The Project Gutenberg EBook of Scientific American Supplement, No. 508,
September 26, 1885, by Various

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Title: Scientific American Supplement, No. 508, September 26, 1885

Author: Various

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Language: English

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[Illustration]




SCIENTIFIC AMERICAN SUPPLEMENT NO. 508




NEW YORK, SEPTEMBER 26, 1885

Scientific American Supplement. Vol. XX., No. 508.

Scientific American established 1845

Scientific American Supplement, $5 a year.

Scientific American and Supplement, $7 a year.

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TABLE OF CONTENTS

                                                                  PAGE
I.   CHEMISTRY AND METALLURGY.--The Cowles Electric Smelting
     Process. 5 figures.                                          8113

     On the Electrical Furnace and the Reduction of the Oxides of
     Boron, Silicon, Aluminum, and other Metals by Carbon.--By
     EUGENE H. COWLES, ALFRED H. COWLES, and CHARLES F. MABERY.   8112

     Chemical Action of Light.                                    8117

     Eutexia.--Cryohydrates.--Eutectic salt alloys and metal
     alloys.                                                      8117

     Chinoline.                                                   8118

     Method of Rapid Estimation of Urea. 1 figure.                8118

     Assay of Earthenware Glaze.                                  8112

II.  ENGINEERING AND MECHANICS.--Deep Shafts and Deep Mining.     8104

     Sinking of the Quievrechain Working Shaft.--Numerous
     figures.                                                     8108

     On the Elementary Principles of the Gas Engine.--An
     interesting paper read before the Gas Institute by Mr.
     DENNY LANE, of Cork, and discussion following.               8109

     M. MEIZEL'S Reciprocating Exhauster.                         8112

     Automatic Siphon for Irrigation. 1 figure.                   8113

III. ELECTRICITY, TELEGRAPHY, ETC.--Optical Telegraphy.--
     Cryptography.--Preservation of Telegrams.--The projector in
     optical telegraphy.--Use of balloons. 4 figures.             8114

     A New Style of Submarine Telegraph. 4 figures.               8115

     A New Circuit Cutter. 2 figures.                             8115

     New Micro Telephonic Apparatus. 5 figures.                   8116

     Messrs. Kapp and Crompton's Measuring Instruments.
     5 figures.                                                   8116

IV.  GEOLOGY, ETC.--Permeability of Sand Rock.--By F.H. NEWELL.   8103

     The Grotto of Gargas, in the Pyrenees.--Paleontological
     remains found therein. 2 engravings.                         8103

     Remarkable Wells and Caverns in Yucatan.--By ALICE D. LE
     PLONGEON.                                                    8105

V.   NATURAL HISTORY.--The Cabbage Butterfly and the Peacock
     Butterfly.                                                   8105

VI.  BOTANY AND HORTICULTURE.--The Bhotan Cypress (Cupressus
     torulosa).--With engraving.                                  8106

     The Pitcher Plant.                                           8106

     What is a Plant?                                             8106

     Camellias.--Culture of the same.                             8106

     Arisaema Fimbriatum.--Leaf, spathe, and floral details.--With
     engraving.                                                   8107

VII. MISCELLANEOUS.--Striking a Light with Bamboo.                8107

     Experiments in Memory.                                       8107

       *       *       *       *       *




PERMEABILITY OF SAND ROCK.

By FREDERICK H. NEWELL, M.E.


Among oil producers, there has been much discussion as to whether the
sand rock in which petroleum occurs is of necessity fissured or is
still in its original unbroken condition.

The earliest and most natural theory, which for years was indisputed,
and is still given by some textbooks, was, that oil wells reached a
cavity filled with petroleum.

Within the past few years, however, the opinion has been gaining
ground that the oil is stored in the sandrock itself in the minute
spaces between the small grains of sand, not entirely filled by
cementing material, and that crevices holding and conducting oil are
rare, all fissures as a rule being confined to the upper fresh-water
bearing rocks of the well. Mr. Carll, in III. Pennsylvania Second
Geological Survey, has discussed this subject very fully, and has made
estimates of the quantity of oil that the sand rock can hold and
deliver into a well; also, T. Sterry Hunt, in his _Chemical and
Geological Essays_, has made deductions as to the petroleum contained
in the Niagara limestone that outcrops about Chicago.

While the experiments and conclusions of these geologists go to prove
that these rocks are capable of holding the oil, there are on record
no facts as to the phenomena of its flow, other than by capillarity,
through the rock. To obtain some data of the flow of liquids under
pressure through certain oil-bearing stones, series of tests on small
pieces were made. These tests were carried on during this spring, and
many results quite unlooked for were obtained. When crude oil,
kerosene, or water (river or distilled) was forced through the
specimens, the pressure being constant, the rate of flow was variable.
At first, the amount flowing through was large, then fell off rapidly,
and when the flow had diminished to about one-quarter of its original
rate, the decrease was very slight, but still continued as long as
measurements were made, in some cases for three weeks.

When using crude oil, this result was not surprising, for, as the oil
men say, crude oil "paraffines up" a rock, that is, clogs the minute
pores by depositing solid paraffine (?); but this so-called
paraffining took place, not only with crude oil, but with refined oil,
and even with distilled water.

The only explanation as yet is, that liquids flowing under pressure
through rock on which they exert little or no dissolving effect,
instead of washing out fine particles, tend to dislodge any minute
grains of the stone that may not be firmly held by cement, and these
block up extremely fine and crooked pores in which the fluid is
passing.

Several tests indicated that this blocking up was largely near the
surface into which the fluid was passing. When this surface was ground
off, even 1/50 of an inch, the flow increased immediately nearly to
the original rate.

Reversing the flow also had the effect of increasing the rate, even
above that of any time previous.

With the moderate pressures used--from 2" to 80" of mercury--the
results show that the rate of flow, other things being equal, is
directly proportional to the pressure.

The porosity of rock is not always a criterion of its permeability; a
very fine grained marble, containing about 0.6 per cent. cell space,
transmitted water and oil more freely than a shale that would hold 4
per cent. of its bulk of water.

If the above conclusions hold on a large scale as on the small, they
may aid in explaining the diminished flow of oil wells. Not only will
the flow lessen from reduced gas pressure, but the passages in the
rock become less able to allow the oil to flow through.

The increase in flow following the explosion of large shots in a sand
rock may be due not only to fissuring of the rock, but to temporary
reversal of the pressure, the force of the explosive tending to drive
the oil back for an instant.

The large shots now used (up to 200 quarts, or say 660 pounds of
nitroglycerine) must exert some influence of this kind, especially
when held down by 500+- feet of liquid tamping. In the course of these
tests, it was noticed that fresh water has a more energetic
disintegrating action on the shales and clay than on salt water.

This may furnish a reason for the fact, noticed by the oil men, that
fresh water has a much more injurious effect than salt in clogging a
well. No oil-bearing sand rock is free from laminae of shale, and when
fresh water gets down into the sand, the water must, as the
experiments show, rapidly break up the shale, setting free fine
particles, which soon are driven along into the minute interstices of
the sand rock, plastering it up and injuring the well.--_Engineering
and Mining Journal._

       *       *       *       *       *




THE GROTTO OF GARGAS.


The grotto of Gargas is located in Mount Tibiran about three hundred
yards above the level of the valley, and about two miles southeast of
the village of Aventignan. Access to it is easy, since a road made by
Mr. Borderes in 1884 allows carriages to reach its entrance.

This grotto is one of the most beautiful in the Pyrenees, and presents
to the visitor a succession of vast halls with roofs that are curved
like a dome, or are in the form of an ogive, or are as flat as a
ceiling. It is easy to explore these halls, for the floor is covered
with a thick stalagmitic stratum, and is not irregular as in the
majority of large caves.

[Illustration: FIG. 1.--SECTION OF THE GROTTO OF GARGAS.]

Upon entering through the iron gate at the mouth of the grotto, one
finds himself in Bear Hall, wherein a strange calcareous concretion
offers the form of the carnivorous animal after which the room is
named. This chamber is about 80 feet in width by 98 in length. We
first descend a slope formed of earth and debris mostly derived from
the outside. This slope, in which are cut several steps, rests upon a
hard, compact, and crystalline stalagmitic floor. Upon turning to the
right, we come to the Hall of Columns, the most beautiful of all. Here
the floor bristles with stalagmites, which in several places are
connected with the stalactites that depend from the ceiling. This room
is about 50 feet square. After this we reach the Hall of Crevices, 80
feet square, and this leads to the great Hall of Gargas, which is
about 328 feet in length by 80, 98, and 105 in width. In certain
places enormous fissures in the vault rise to a great height. Some of
these, shaped like great inverted funnels, are more than 60 yards in
length. The grotto terminates in the Creeping Hall. As its name
indicates, this part of the cave can only be traversed by lying flat
upon the belly. It gives access to the upper grotto through a narrow
and difficult passage that it would be possible to widen, and which
would then allow visitors to make their exit by traversing the
beautiful upper grotto, whose natural entrance is situated 150 yards
above the present one. This latter was blasted out about thirty years
ago.

Upon following the direction of the great crevices, we reach a small
chamber, wherein are found the Oubliettes of Gargas--a vertical well
65 feet feet in depth. The aperture that gives access to this strange
well (rendered important through the paleontological remains collected
in it) is no more than two feet in diameter. Such is the general
configuration of the grotto.

In 1865 Dr. Garrigou and Mr. De Chastaignier visited the grotto, and
were the first to make excavations therein. These latter allowed these
scientists to ascertain that the great chamber contained the remains
of a quaternary fauna, and, near the declivity, a deposit of the
reindeer age.

As soon as it was possible to obtain a permit from the Municipal
Council of Aventignan to do so, I began the work of excavation, and
the persistence with which I continued my explorations led me to
discover one of the most important deposits that we possess in the
chain of the Pyrenees. My first excavations in Bear Hall were made in
1873, and were particularly fruitful in an opening 29 feet long by 10
wide that terminates the hall, to the left. I have remarked that these
sorts of retreats in grottoes are generally rich in bones. Currents of
water rushing through the entrance to the grotto carry along the
bones--entire, broken, or gnawed--that lie upon the ground. These
remains are transported to the depths of the cave, and are often
stopped along the walls, and lie buried in the chambers in
argillaceous mud. Rounded flint stones are constantly associated with
the bones, and the latter are always in great disorder. The species
that I met with were as follows: the great cave bear, the little bear,
the hyena, the great cat, the rhinoceros, the ox, the horse, and the
stag.

The stalagmitic floor is 11/2, 2, and 21/4 inches thick. The bones were
either scattered or accumulated at certain points. They were generally
broken, and often worn and rounded. They appeared to have been rolled
with violence by the waters. The clay that contained them was from 3
to 6 feet in thickness, and rested upon a stratum of water-worn
pebbles whose dimensions varied from the size of the fist to a grain
of sand. A thick layer of very hard, crystalline stalagmite covers the
Hall of Columns, and it was very difficult to excavate without
destroying this part of the grotto.

I found that there anciently existed several apertures that are now
sealed up, either by calcareous concretions or by earthy rubbish from
the mountain. One of these was situated in the vicinity of the present
mouth, and permitted of the access to Bear Hall of a host of carnivora
that found therein a vast and convenient place of shelter.

[Illustration: FIG. 2.--SKELETON OF THE CAVE HYENA.]

These excavations revealed to me at this entrance, at the bottom of
the declivity, a thick stratum of remains brought thither by primitive
man. This deposit, which was formed of black earth mixed with charcoal
and numerous remains of bones, calcined and broken longitudinally for
the most part, contained rudely worked flint stones. I collected a few
implements, one surface of which offered a clean fracture, while the
other represented the cutting edge. According to Mr. De Mortillet,
such instruments were not intended to have a handle. They were capable
of serving as paring knives and saws, but they were especially
designed for scraping bones and skins. The deposit was from 26 to 32
feet square and from 2 inches to 5 feet deep, and rested upon a bed of
broken stones above the stalagmite. The animals found in it were the
modern bear (rare), the aurochs, the ox, the horse, and the stag--the
last four in abundance.

At the extremity of the grotto there is a well with vertical sides
which is no less than 65 feet in depth. It is called the Gargas
Oubilettes. Its mouth is from 15 to 24 inches in diameter, and
scarcely gives passage to a man (Fig. 1). Mr. Borderes, in the hope of
discovering a new grotto, was the first to descend into this well,
which he did by means of a rope ladder, and collected a few bones that
were a revelation to me. Despite the great difficulty and danger of
excavating at this point, I proceeded, and found at the first blow of
the pick that there was here a deposit of the highest importance,
since all the bones that I met with were intact. The first thing
collected was an entire skull of the great cave bear, with its
maxillaries in place. From this moment I began a series of excavations
that lasted two years.

The descent is effected through a narrow vertical passage 61/2 feet in
length. The cavity afterward imperceptibly widens, and, at a depth of
12 yards, reaches 61/2 feet in diameter, and at 15 yards 10 feet.
Finally, in the widest part (at a depth of 62 feet) it measures about
16 feet (Fig. 1).

A glance at the section of the well, which I have drawn as accurately
as possible (not an easy thing to do when one is standing upon a rope
ladder), will give an idea of the form of this strange pocket formed
in the limestone of the mountain through the most complex dislocations
and erosions. Two lateral pockets attracted my attention because of
the enormous quantity of clay and bones that obstructed them. The
first, to the left, was about 15 feet from the orifice. When we had
entirely emptied it, we found that it communicated with the bottom of
the well by a narrow passage. An entire skeleton of the great cave
bear had stopped up this narrow passage, and of this, by the aid of a
small ladder, we gathered the greater part of the skeleton, the state
of preservation of which was remarkable.

The second pocket, which was almost completely filled with clay, and
situated a little lower than the other, likewise communicated with a
third cavity that reached the bottom of the well. The clay of these
different pockets contained so large a quantity of bones that we could
hardly use our picks, and the excavation had to be performed with very
short hooks, and often by hand. In this way I was enabled to remove
the bones without accident. The lower pocket was dug out first, and
with extreme care, the bones being hoisted out by means of a basket
attached to a rope. Three or four candles sufficed to give us light.
The air was heavy and very warm, and, after staying in it for two
hours, it was necessary to come to the surface to breathe. After
extracting the bones from the lower pocket, and when no more clay
remained, we successively dug out the upper ones and threw the earth
to the bottom of the well.

On the 20th of December, 1884, my excavating was finished. To-day the
Oubliettes of Gargas are obstructed with the clay that it was
impossible to carry elsewhere. The animals that I thus collected in
the well were the following: The great bear (in abundance), the little
bear (a variety of the preceding), the hyena, and the wolf. The
pockets contained nearly entire skeletons of these species. How had
the animals been able to penetrate this well? It is difficult to admit
that it was through the aperture that I have mentioned. I endeavored
to ascertain whether there was not another communication with the
Gargas grotto, and had the satisfaction of finding a fissure that
ended in the cave, and that probably was wider at the epoch at which
the place served as a lair for the bear and hyena.

Very old individuals and other adults, and very young animals, were
living in the grotto, and, being surprised, without power to save
themselves, by a sudden inundation, reached the bottom of the well
that we have described. The entire remains of these animals were
carried along by the water and deposited in the pockets in the rock.
Once buried in the argillaceous mud, the bones no longer underwent the
action of the running water, and their preservation was thence
secured.--_F. Regnault, in La Nature._

       *       *       *       *       *




DEEP SHAFTS AND DEEP MINING.


A correspondent of the New York _Sun_, writing from Virginia City,
Nevada, describes the progress of the work there on the Combination
shaft of the Comstock lode, the deepest vertical shaft in America, and
the second deepest in the world. It is being sunk by the Chollar
Potosi, Hale & Norcross, and Savage mining companies; hence its name
of the Combination shaft. This shaft has now reached a perpendicular
depth of a little over 3,100 feet. There is only one deeper vertical
shaft in the world--the Adalbent shaft of the silver-lead mines of
Przibram, Bohemia, which at last accounts had reached a depth of 3,280
feet. The attainment of that depth was made the occasion of a
festival, which continued three days, and was still further honored by
the striking off of commemorative medals of the value of a florin
each. There is no record of the beginning of work on this mine at
Przibram, although its written history goes back to 1527.

Twenty years ago very few mining shafts in the world had reached a
depth of 2,000 feet. The very deepest at that time was in a
metalliferous mine in Hanover, which had been carried down 2,900 feet;
but this was probably not a single perpendicular shaft. Two vertical
shafts near Gilly, in Belgium, are sunk to the depth of 2,847 feet. At
this point they are connected by a drift, from which an exploring
shaft or winze is sunk to a further depth of 666 feet, and from that
again was put down a bore hole 49 feet in depth, making the total
depth reached 3,562 feet. As the bore hole did not reach the seam of
coal sought for, they returned and resumed operations at the 2,847
level. In Europe it is thought worthy of particular note that there
are vertical shafts of the following depths:

                                                     Feet.
  Eimkert's shaft of the Luganer Coal Mining
          Company, Saxony                            2,653

  Sampson shaft of the Oberhartz silver mine,
          near St. Andreasberg, Hanover.             2,437

  The hoisting shaft of the Rosebridge Colliery,
          near Wigan, Lancashire, England.           2,458

  Shaft of the coal mines of St. Luke, near
          St. Chaumont, France.                      2,253

  Amelia shaft, Shemnitz, Hungary.                   1,782

  The No. 1 Camphausen shaft, near Fishbach,
          in the department of the Saarbruck
          Collieries, Prussia.                       1,650


Now, taking the mines of the Comstock for a distance of over a
mile--from the Utah on the north to the Alto on the south--there is
hardly a mine that is not down over 2,500 feet, and most of the shafts
are deeper than those mentioned above; while the Union Consolidated
shaft has a vertical depth of 2,900 feet, and the Yellow Jacket a
depth of 3,030 feet. In his closing argument before the Congressional
Committee on Mines and Mining in 1872, Adolph Sutro of the Sutro
tunnel said: "The deepest hole dug by man since the world has existed
is only 2,700 feet deep, and it remains for the youngest nation on
earth to contribute more to science and geology by giving
opportunities of studying the formation of mineral veins at a greater
depth than has ever been accomplished by any other nation in the
world." Mr. Sutro was of the opinion that the completion of his tunnel
would enable our leading mining companies to reach a vertical depth of
5,000 feet.

This great depth has never yet been attained except in a bore hole or
artesian well. The deepest points to which the crust of the earth has
ever been penetrated have been by means of such borings in quest of
salt, coal, or water. A bore hole for salt at Probst Jesar, near
Lubtheen, for the Government of Mecklenberg-Schwerin, is down 3,315
feet, the size of which bore is twelve inches at the top and three
inches at the bottom. A bore hole was put down for the Prussian
Government to the depth of 4,183 feet. But in these bore holes the
United States leads the world, as there is one near St. Louis, Mo.,
that is 5,500 feet in depth. Here on the Comstock, in the Union
Consolidated mine, a depth of 3,300 feet has been attained, but not by
means of a single vertical shaft. The vertical depth of the shaft is
2,900 feet; the remainder of the depth has been attained by means of
winzes sunk from drifts. Several long drifts were run at this great
depth without difficulty as regards ventilation or heat.

The combination shaft is situated much further east (in which
direction the lode dips) than any other on the Comstock. It is 3,000
feet east of the point where the great vein crops out on the side of
Mount Davidson; 2,200 feet east of the old Chollar-Potosi shaft, 1,800
ft. east of the old Hale & Norcross (or Fair) shaft, and 2,000 ft.
east of the Savage shaft. Thus, it will be seen it is far out to the
front in the country toward which the vein is going. The shaft is sunk
in a very hard rock (andesite), every foot of which requires to be
blasted. The opening is about thirty feet in length by ten feet in
width. In timbering up this is divided into four different
compartments, some for the hoisting and some for the pumping
machinery, thus presenting the appearance at the top of four small
shafts set in a row. Over the shaft stand several large buildings, all
filled with ponderous machinery.

The Sutro drain tunnel (nearly four miles in length) connects with the
shaft at a depth of 1,600 ft., up to which point all the water
encountered below is pumped. The shaft was sunk to the depth of 2,200
ft. before more water was encountered than could be hoisted out in the
"skips" with the dirt. At the 2,200 level two Cornish pumps, each with
columns fifteen inches in diameter, were put in. At the 2,400 level
the same pumps were used. On this level a drift was run that connected
with the old Hale & Norcross and Savage shafts, producing a good
circulation of air both in the shaft and in the mines mentioned. At
this point, on account of the inflow from the mines consequent upon
connecting with them by means of the drift, they had more water than
the Cornish pumps could handle, and introduced the hydraulic pumps,
which pumps are run by the pressure of water from the surface through
a pipe running down from the top of the shaft, whereas the Cornish
pumps are run by huge steam engines.

By means of the hydraulic pumps they were enabled to sink the shaft to
the 2,600 level, and extended the Cornish pumps to that point, where
another set of hydraulic pumps was put in. They then sunk the shaft to
the 2,800 level, when they ran another drift westward, and tapped the
vein. The prospects at this depth in the Hale & Norcross and Chollar
mines were so encouraging that the management decided to sink the
shaft to the depth of 3,000 ft. On reaching the 3,000 level, they ran
a third drift through to the vein. The distance from the shaft to the
east wall of the vein was found to be only 250 ft. At the depth of
3,000 ft. they put in one of the pair of hydraulic pumps that is to be
set up there. The second pump is now arriving from San Francisco, and
as soon as the several parts are on the ground, it will be at once put
in place alongside its fellow on the 3,000 level. This additional pump
will increase the capacity from 600,000 to 700,000 gallons in
twenty-four hours, or about forty-five miners' inches.

Owing to the excellent showing of ore obtained on the 3,000 level by
the Hale & Norcross Company, and to the continuation of the ore below
that level (as shown by a winze sunk in the vein), the management
determined to sink the shaft to the vertical depth of 3,200 ft. It is
now 3,120 ft. deep, and it is safe to say that it will reach the depth
of 3,200 ft. early in September, when it will lack but eighty feet of
being as deep as the shaft at Przibram was at the time of the great
festival. Although the shaft is of great size--about thirty feet by
ten feet before the timbers are put in--the workmen lower it at the
rate of about three feet a day, in rock as hard as flint.

The hydraulic pump now working at the 3,000 foot level of the shaft is
the deepest in the world. In Europe the deepest is in a mine in the
Hartz Mountains, Germany, which is working at the depth of 2,700 feet.
It is, however, a small pump not half the size of the one in the
Combination shaft. Although these pumps were first used in Europe,
those in operation here are far superior in size, and in every other
respect, to those of the Old World, several valuable improvements
having been made in them by the machinists of the Pacific coast.

The capacity of the two Cornish pumps, which lift the water from the
2,900 foot level to the Sutro drain tunnel (at the 1,600 level), is
about 1,000,000 gallons in twenty-four hours, and the capacity of the
present hydraulic pumps is 3,500,000 gallons in the same time. They
are now daily pumping, with both hydraulic and Cornish pumps, about
4,000,000 gallons, but could pump at least 500,000 gallons more in
twenty-four hours than they are now doing. The daily capacity with the
hydraulic pump now coming, and which will be set up as mate to that
now in operation at the 3,000 foot level, will be 5,200,000 gallons.

The water which feeds the pressure pipe of the three sets of hydraulic
pumps is brought from near Lake Tahoe, in the Sierra Nevada Mountains.
The distance is about thirty miles, and the greater part of the way
the water flows through iron pipes, which at one point cross a
depression 1,720 feet in depth. The pressure pipe takes this water
from a tank situated on the eastern slope of Mount Davidson, 3,500
feet west of the shaft. At the tank this pipe is twelve inches in
diameter, but is only eight inches where it enters the top of the
shaft. The tank whence the water is taken is 426 feet higher than the
top of the shaft, therefore the vertical pressure upon the hydraulic
pump at the 3,000 foot level is 3,426 feet. The pressure pipe is of
ordinary galvanized iron where it receives the water at the tank, but
gradually grows thicker and stronger, and at the 3,000 level it is
constructed of cast iron, and is 21/2 inches in thickness. The pressure
at this point is 1,500 pounds to the square inch.

In the early days of hydraulic mining in California the miners thought
that with a vertical pressure of 300 feet they could almost tear the
world to pieces, and not a man among them could have been made to
believe that any pipe could be constructed that would withstand a
vertical pressure of 1,000 feet; but we now see that a thickness of
two and a half inches of cast iron will sustain a vertical pressure of
over 3,400 feet.

There is only one pressure pipe for all the hydraulic pumps. This
extends from the tank on the side of the mountain to the 3,000 foot
level. It is tapped at the points where are situated the several sets
of hydraulic pumps. The water from the pressure pipe enters one part
of the pump, where it moves a piston-back and forth, just as the
piston of a steam engine is moved by steam. This water engine moves a
pump which not only raises to the surface the water which has been
used as driving power, but also a vast quantity of water from the
shaft, all of which is forced up to the Sutro drain tunnel through
what is called a return pipe. Each set of hydraulic pumps has its
return pipe; therefore there are three return pipes--one from the
2,400, one from the 2,600, and another from the 3,000 level.

Some idea may be formed of the great size of these hydraulic engines
when it is known that the stations excavated for them at the several
levels where they are placed are 85 feet long, 28 feet wide, and 12
feet high. All this space is so filled with machinery that only
sufficient room is left to allow of the workmen moving about it. One
of these stations would, on the surface, form a hall large enough for
a ball room, and to those who are unacquainted with the skill of our
miners it must seem wonderful that such great openings can be made and
securely supported far down in the bowels of the earth; yet it is very
effectually done. These great subterranean halls are supported by
timbers 14x16 inches square set along the walls three feet apart, from
center to center, and the caps or joists passing overhead are timbers
of the same size. The timber used is mountain spruce. Not one of these
huge stations has thus far cost one dollar for repairs. The station at
the 2,400 level has been in use five years, that at the 2,600 three
years, and the one at the 3,000 level eight months. Room for
ventilation is left behind the timbers, and all are still sound.
Timbers of the same kind are used in the shaft, and all are sound. The
shaft has cost nothing for repairs. Being in hard andesite rock from
top to bottom, the ground does not swell and crowd upon the timbers.

If it shall be thought advisable to go to a greater depth than 3,200
feet, a station of large size will be made on the east side of the
present shaft, and in this station will be sunk a shaft of smaller
size. The reason why the work will be continued in this way is that in
a single hoist of 3,200 feet the weight of a steel wire cable of that
length is very great--so great that the loaded cage it brings up is a
mere trifle in comparison. In this secondary shaft the hoisting
apparatus and pumps will be run by means of compressed air. As it is
very expensive to make compressed air by steam power, the pressure
pipe will be tapped at the level of the Sutro tunnel, and a stream of
water taken out that will be used in running a turbine wheel of
sufficient capacity to drive three air compressors. As there will be a
vertical pressure upon the turbine at this depth of over 2,000 feet, a
large stream of water will not be required. The water used in driving
the wheel will flow out through the Sutro tunnel, and give no trouble
in the shaft.

By means of this great shaft and its powerful hydraulic and Cornish
pumps the crust of the earth will probably yet be penetrated to far
greater depth than in any other place in the world. It has been only a
little over ten years since the work of sinking it was begun, whereas
in the mines of the Old World they have been delving since "time
whereof the memory of man runneth not to the contrary." The work on
the Combination shaft has been by no means continuous. There have been
long stoppages aside from those required at such times as they were
engaged in running long drifts to the westward to tap the vein, and at
times for many months, when the several companies interested in the
shaft were engaged in prospecting the various levels it had opened up.

       *       *       *       *       *




REMARKABLE WELLS AND CAVERNS.


Yucatan is one of the most interesting States of Mexico, owing to the
splendid ancient palaces and temples of once grand cities, now hidden
in the forests. That country also presents great attractions for
geologists and botanists, as well as naturalists, who there find rare
and beautiful birds, insects, and reptiles.

There are no rivers on the surface of the land, but in many parts it
is entirely undermined by extensive caverns, in which are basins of
water fed by subterranean currents. The caverns are delightfully cool
even at midday, and the fantastic forms of some of the stalactites and
stalagmites are a never-ending source of interest. There are long
winding passages and roomy chambers following one after another for
great distances, with here and there some chink in the stony vault
above, through which a sunbeam penetrates, enabling us to see to the
right and left openings leading to untrodden places in the bowels of
the earth. As few of these caves have been explored, the wildest
accounts are given by the natives concerning the dark recesses where
only wild beasts seek shelter. Before venturing far in, it is
advisable to secure one end of a ball of twine at the entrance, and
keep the ball in hand; nor is it safe to go without lanterns or
torches, lest we step into some yawning chasm or deep water. The
leader of one party suddenly saw a very dark spot just before him; he
jumped over, instead of stepping on it, and told the others to halt.
Examination proved the dark patch to be a pit that seemed bottomless.

Awe-inspiring as are the interiors of some of these caves, they are
frequently most beautiful. The natural pillars are often grand in
dimensions and sparkling with various hues, while stalactites and
stalagmites sometimes resemble familiar objects with astonishing
perfection. It is, however, not advisable to place implicit confidence
in accounts of the natives, for the reality, no matter how beautiful,
can hardly be equal to what the vivid imagination of the Indian has
pictured. Anything bearing the least resemblance to a woman is called
"a most beautiful Virgin Mary." Fantastic flutings become "an organ,"
and a level rock "an altar." Only once we were not disappointed, when,
having been told to look for a pulpit, we found one that appeared as
if man must have fashioned it, supported on a slender pyramidal base,
the upper part very symmetrical, and ornamented with a perfect
imitation of bunches of grapes and other fruit.

As I have already said, in these caves are sheets of water, some very
large, others only a few feet in circumference, fed by subterranean
currents. When the water is clear and sweet, it is peopled by a kind
of bagre, a blind fish called by the natives _tzau_, also a species of
_Silurus_. But there are likewise medicinal and thermal waters, by
bathing in which many people claim to have been cured of most painful
and obstinate diseases.

Strange stories are told of some of these waters. Of one it is said
that those who approach it without holding their breath fall dead.
People who live near the place swear it is so, and say the water
appears to boil on such occasions. From the thermal waters, in some
cases 100 feet below the soil, and without means of access except by
buckets let down through an opening in the rock, warm vapors issue at
early morn, but when the sun is high the water is cool and pleasant to
drink.

The name _senote_ is given to all these deposits of water, also to
some immense natural circular wells from 50 to 300 feet in diameter.
The walls are more or less perpendicular, generally covered with
tropical vegetation. The current in some is swift, but no inlets or
outlets are visible. The water is deliciously pure and sweet, much
better than that of wells opened by man in the same country. These
enormous deposits generally have a rugged path, sometimes very steep,
leading to the water's edge, but daring natives throw themselves from
the brink, afterward ascending by stout roots that hang like ropes
down the walls, the trees above sucking through these roots the
life-sustaining fluid more than a hundred feet below.

In the west part of Yucatan is a village called _Bolonchen_ (nine
wells), because in the public square there are nine circular openings
cut through a stratum of rock. They are mouths of one immense cistern,
if natural or made by hand the natives do not know, but in times of
drought it is empty, which shows that it is not supplied by any
subterranean spring. Then the people depend entirely on water found in
a cave a mile and a half from the village; it is perhaps the most
remarkable cavern in the whole country. The entrance is magnificently
wild and picturesque. It is necessary to carry torches, for the way is
dark and dangerous. After advancing sixty or seventy feet we descend a
strong but rough ladder twenty feet long, placed against a very
precipitous rock. Not the faintest glimmer of daylight reaches that
spot; but after a while we stand on the brink of a perpendicular
precipice, the bottom of which is strongly illuminated through a hole
in the surface rock more than 200 feet above. Standing on the verge of
this awful pit in the dim light, the rocks and crags seem to take on
most weird shapes. We go down into the great hole by a ladder eighty
feet high and twelve wide, and, reaching the bottom, are as yet but at
the mouth of the cave, which, by the bye, is called _Xtacunbi Xunan_
(the hidden lady), because, say the Indians, a lady was stolen from
her mother and hidden there by her lover. Now, to our right, we find a
narrow passage, and soon another ladder; the darkness is intense and
the descent continuous, though irregular, like a series of hills and
dales, ladders being placed against the steepest places.

After an exhausting journey we reach a vast chamber, from which
crooked passages lead in various directions to wells, seven in all,
each named according to the peculiar kind of water. One, always warm,
is called _Chocoha_ (hot water); another, _O[c]iha_* (milky water), and
_Akabha_ (dark water). About 400 paces away from the chamber, passing
through a very narrow, close passage, there is a basin of red water
that ebbs and flows like the sea, receding with the south wind,
increasing with the northwest.

   *Transcriber's note: [c] denotes upside-down 'c' in original.

To reach the most distant well, we go down yet one more ladder, the
seventh. On one side of it there is a perpendicular wall, on the other
a yawning gulf, so when one of the steps, merely round sticks tied
with withes, gave way beneath our feet, we tightly grasped the stick
above. Having reached the bottom of the ladder, we crawl on our hands
and feet through a broken, winding passage about 800 feet long, then
see before us a basin of crystalline water, and how thirsty we are!
This basin is 1,400 feet from the mouth of the cave, and about 450
feet below the earth's surface. Several hundred people during five
months in every year depend entirely on that source for all the water
they use. With their frail pitchers and flaring torches they wend
their way, gasping for breath, through the intricate passages, and
reaching the water, are so profusely perspiring that they must wait
before quenching their thirst. The way back is even harder, and they
are tired and loaded; yet these people are such lovers of cleanliness
that on their arrival at their poor huts, before tasting food, they
will use some of the water that has cost them so much, to bathe their
smoke-begrimed skin. As several women once fainted in the cave, men
generally fetch the water now.

Yucatan is, and has been for ages past, quite free from earthquakes,
while all surrounding countries are from time to time convulsed. This
immunity may be due to the vast caverns and numerous great wells
existing throughout the land. Pliny the Elder was of opinion that if
numerous deep wells were made in the earth to serve as outlets for the
gases that disturb its upper strata, the strength of the earthquakes
would be diminished, and if we may judge by Yucatan, Pliny was right
in his conjectures. After him, other scientists who have carefully
studied the subject have expressed the same opinion with regard to the
efficacy of large wells.

ALICE D. LE PLONGEON.

Brooklyn, July 15, 1885.

       *       *       *       *       *


Cholera failed to strike a single one of the 4,000 women employed in
the national tobacco factory at Valencia, Spain, though the disease
raged violently in that city, and the _Medical World_ recalls that
tobacco workers were also noticed to enjoy exemption from attack
during an epidemic at Amsterdam.

       *       *       *       *       *




THE CABBAGE BUTTERFLY.


A patch of eggs and the minute caterpillars or larvae nearly emerged
from them are seen on the leaf. These tiny eggs are at first quite
white or pale yellow, and form an object for the microscope of
remarkable beauty, which is worthy of the examination of all who take
an interest in the garden and its insect life. An egg magnified is
drawn at the bottom left-hand corner of the woodcut. When the eggs are
near the hatching point they darken in color, and a magnifying glass
reveals through the delicate transparent shell a sight which fills the
observer with amazement; the embryo caterpillar is seen in gradual
course of formation, and if patience and warmth have permitted it, the
observer will witness slight movements within the life-case, and
presently the shell will break and a black head with moving jaws will
be thrust out; the little caterpillar unfolds and slowly crawls away
from the egg-shell, and inserts its jaws into the green leaf. It is
curious to witness how judiciously the little creatures avoid crowding
together, but strike out in different directions, and thus they make
sure of a plentiful supply of food, and distribute the effects of
their depredations. These caterpillars eat continually, and hence
rapidly increase in size, until they present the appearance shown in
our drawing at the bottom of the illustration, which is a full grown
caterpillar.

[Illustration: THE CABBAGE AND PEACOCK BUTTERFLIES.]

It will be observed that this insect is composed of thirteen segments
from head to tail, which is a distinctive characteristic of all
insects both in the larval and perfect states; but in the case of this
and most other caterpillars these segments are sharply defined and
readily recognized. It will also be noticed that the three segments or
"joints" nearest the head bear a pair of legs each; these are the real
feet, or claspers, as they are sometimes termed, which develop into
the feet of the future butterfly. There are four pairs of false feet
or suckers, which adhere to the ground by suction, and which disappear
in the butterfly. On the last or tail end is a fifth pair of suckers
also, which can attach themselves to a surface with considerable
force, as any one can attest who has noticed the wrigglings of one of
these caterpillars when feeling for new feeding ground.

The caterpillar now ceases to eat, and quietly betakes itself to a
secluded corner, where in peace it spins a web around its body, and
wrapt therein remains quiescent, awaiting its change into the
butterfly. Although so dormant outwardly, activity reigns inside;
processes are going on within that chrysalis-case which are the
amazement and the puzzle of all naturalists. In course of time the
worm is changed into the beautiful winged butterfly, which breaks its
case and emerges soft and wet; but it quickly dries and spreads its
wings to commence its life in the air and sunshine. The chrysalis is
represented in the figure on the left. The butterfly, it will be
recognized, is one of the common insects so familiar to all, with
strongly veined white wings, bearing three black spots, two on the
upper and one on the lower wing, and dark coloring on the corner of
the upper wings. The antennae, as with all butterflies, are clubbed at
the extremity--unlike moths', which are tapering--and the large black
staring eyes are the optical apparatus, containing, we are told,
thousands of lenses, each a perfect, simple eye.

The wings derive their chief coloring from the covering of scales,
which lie on like slates on a roof, and are attached in a similar
manner. A small portion of the wing magnified is represented at the
bottom right hand corner, and detached scales more highly magnified
next to it, exhibiting somewhat the form of battledoors.


THE PEACOCK BUTTERFLY.

Another well known insect is illustrated in the figure in the upper
portion--the peacock butterfly (Vanessa Io). The curious spiked and
spotted caterpillar feeds upon the common nettle. This beautiful
butterfly--common in most districts--is brilliantly colored and
figured on the upper side of the wings, but only of a mottled brown on
the under surface, somewhat resembling a dried and brown leaf, so that
it is no easy matter to detect the conspicuous, brightly-decked insect
when it alights from flight upon foliage, and brings its wings
together over its back after the manner of butterflies. At the
left-hand corner is seen the head of the insect, magnified, showing
the long spiral tongue.

This is a curious structure, and one that will repay the trouble of
microscopic examination. In the figure the profile is seen, the large
compound eye at the side and the long curved tongue, so
elephantine-looking in form, though of minute size, is seen unrolled
as it is when about to be inserted into flowers to pump up the
honey-juice. This little piece of insect apparatus is a mass of
muscles and sensitive nerves comprising a machine of greater
complexity and of no less precision in its action than the modern
printing machine. When not in use, the tongue rolls into a spiral and
disappears under the head. A butterfly's tongue may readily be
unrolled by carefully inserting a pin within the first spiral and
gently drawing it out.--_The Gardeners' Chronicle._

       *       *       *       *       *




THE BHOTAN CYPRESS.

(CUPRESSUS TORULOSA.)


This cypress, apart from its elegant growth, is interesting as being
the only species of Cupressus indigenous to India. It is a native of
the Himalayas in the Bhotan district, and it also occurs on the
borders of Chinese Tartary. It forms, therefore, a connecting link, as
it were, between the true cypresses of the extreme east and those that
are natives of Europe. It is singular to note that this genus of
conifers extends throughout the entire breadth of the northern
hemisphere, Cupressus funebris representing the extreme east in China,
and C. macrocarpa the extreme west on the Californian seacoast. The
northerly and southerly limits, it is interesting to mark, are, on the
contrary, singularly restricted, the most southerly being found in
Mexico; the most northerly (C. nutkaensis) in Nootka Sound, and the
subject of these remarks (C. torulosa) in Bhotan. The whole of the
regions intervening between these extreme lateral points have their
cypresses. The European species are C. lusitanica (the cedar of Goa),
which inhabits Spain and Portugal; C. sempervirens (the Roman
cypress), which is centered chiefly in the southeasterly parts of
Europe, extending into Asia Minor. Farther eastward C. torulosa is met
with, and the chain is extended eastward by C. funebris, also known as
C. pendula. The headquarters of the cypresses are undoubtedly in the
extreme west, for here may be found some four or five distinct
species, including the well-known C. Lawsoniana, probably the most
popular of all coniferae in gardens, C. Goveniana, C. Macnabiana, C.
macrocarpa, and C. nutkaensis (spelt C. nutkanus by the Californian
botanists). The eastern representative of the cypresses in the United
States of North America is C. thyoides, popularly known as the white
cedar. In Mexico three or four species occur, so that the genus in
round numbers only contains about a dozen species. The Californian
botanist Mr. Sereno Watson takes away Lawson's cypress from Cupressus
and puts it in the genus Chamaecyparis, the chief points of distinction
being the flattened two-ranked branchlets and the small globose cones
maturing the first year.

[Illustration: CONES OF CUPRESSUS TORULOSA (NATURAL SIZE).]

All the cypresses are undoubtedly valuable from a garden point of
view, but the various species vary in degree as regards their utility
as ornamental subjects. I should rank them in the following order in
point of merit: C. Lawsoniana, C. nutkaensis, C. macrocarpa, C.
sempervirens, C. thyoides, C. Macnabiana, and C. Goveniana; then would
follow C. torulosa, C. funebris, C. Knightiana, and other Mexican
species. These are placed last, not because they are less elegant than
the others, but on account of their tenderness, all being liable to
succumb to our damp and cold winters. The species which concerns us at
present, C. torulosa, is an old introduction, seeds of it having been
sent to this country by Wallich so long back as 1824, and previous to
this date it was found by Royle on the Himalayas, growing at
elevations of some 11,500 feet above sea level. Coming from such a
height, one would suppose it to be hardier than it really is, but its
tenderness may probably be accounted for by the wood not getting
thoroughly ripened during our summers. It is a very handsome tree,
said to reach from 20 feet to 125 feet in height in its native
habitat. It has a perfectly straight stem; the growth is pyramidal or
rather conical, and the old wood is of a warm purplish-brown. The
foliage is a glaucous gray-green, and the branches have a twisted and
tufted appearance.

There are several varieties of it which are, or have been, in
cultivation. Of these one of the best is corneyana, which Gordon
ranked as a distinct species. It was supposed to be Chinese, and was
introduced to cultivation by Messrs. Knight & Perry, the predecessors
of Messrs. Veitch at the Chelsea Nurseries. It differs from C.
torulosa proper, its habit being of low stature, and has slender
pendulous branches; hence, it has been known in gardens by the names
of C. gracilis, C. cernua, and C. pendula. Other varieties of C.
torulosa are those named in gardens and nurseries--viridis, a kind
devoid of the glaucous foliage of the original; majestica, a robust
variety; and nana, a very dwarf and compact-growing sort. There is
also a so-called variegated form, but it is not worthy of mention. The
synonyms of C. torulosa itself are C. cashmeriana, C. nepalensis, and
C. pendula. Having regard to the tenderness of this Bhotan cypress, it
should only be planted in the warmest localities, and in dry sheltered
positions; upland districts, too, provided they are sheltered, are
undoubtedly suitable for it, inasmuch as growth is retarded in spring,
and, therefore, the young shoots escape injury from late spring
frosts.--_W.G., in The Garden._

       *       *       *       *       *




THE PITCHER PLANT.


The variety of the pitcher plant (_Sarracenia variolaris_) found in
North America is carnivorous, being a feeder on various animal
substances.

Mrs. Mary Treat, an American naturalist, made, a few years ago,
several experiments upon the plants of this species to be found in
Florida; and to the labors of this lady the writer has been indebted,
in some measure, in the preparation of this paper.

The _Sarracenia_ derives its name of "pitcher plant" from the fact of
its possessing the following curious characteristics: The median nerve
is prolonged beyond the leaves in the manner of a tendril, and
terminates in a species of cup or urn. This cup is ordinarily three or
four inches in depth, and one to one and a half inches in width. The
orifice of the cup is covered with a lid, which opens and shuts at
certain periods. At sunrise the cup is found filled with sweet, limpid
water, at which time the lid is down. In the course of the day the lid
opens, when nearly half the water is evaporated; but during the night
this loss is made up, and the next morning the cup is again quite
full, and the lid is shut.

About the middle of March the plants put forth their leaves, which are
from six to twelve inches long, hollow, and shaped something like a
trumpet, while the aperture of the apex is formed almost precisely in
the same manner as those of the plants previously described. A broad
wing extends along one side of the leaf, from the base to the opening
at the top; this wing is bound or edged with a purple cord, which
extends likewise around the cup. This cord secretes a sweet fluid, and
not only flying insects, but those also that crawl upon the ground,
are attracted by it to the plants. Ants, especially, are very fond of
this fluid, so that a line of aphides, extending from the base to the
summit of a leaf, may frequently be observed slowly advancing toward
the orifice of the cup, down which they disappear, never to return.
Flying insects of every kind are equally drawn to the plant; and
directly they taste the fluid, they act very curiously. After feeding
upon the secretions for two or three minutes they become quite stupid,
unsteady on their feet, and while trying to pass their legs over their
wings to clear them, they fall down.

It is of no use to liberate any of the smaller insects; every fly,
removed from the leaf upon which it had been feeding, returned
immediately it was at liberty to do so, and walked down the fatal cup
as though drawn to it by a species of irresistible fascination.

It is not alone that flies and other small insects are overpowered by
the fluid which exudes from the cord in question. Even large insects
succumb to it, although of course not so quickly. Mrs. Treat says: "A
large cockroach was feeding on the secretion of a fresh leaf, which
had caught but little or no prey. After feeding a short time the
insect went down the tube so tight that I could not dislodge it, even
when turning the leaf upside down and knocking it quite hard. It was
late in the evening when I observed it enter; the next morning I cut
the tube open; the cockroach was still alive, but it was covered with
a secretion produced from the inner surface of the tube, and its legs
fell off as I extricated it. From all appearance the terrible
_Sarracenia_ was eating its victim alive. And yet, perhaps, I should
not say 'terrible,' for the plant seems to supply its victims with a
Lethe-like draught before devouring them."

If only a few insects alight upon a leaf, no unpleasant smell is
perceptible during or after the process of digestion; but if a large
number of them be caught, which is commonly the case, a most offensive
odor emanates from the cup, although the putrid matter does not appear
to injure in any manner the inner surface of the tube, food, even in
this condition, being readily absorbed, and going to nourish the
plant. In fact, it would seem that the _Sarracenia_, like some
animals, can feed upon carrion and thrive upon it.

In instances in which experiments have been made with fresh, raw beef
or mutton, the meat has been covered in a few hours with the
secretions of the leaves, and the blood extracted from it. There is,
however, one difference between the digesting powers of the leaves
when exercised upon insects or upon meat. Even if the bodies of
insects have become putrid, the plant, as has already been stated, has
no difficulty in assimilating them; but as regards meat, it is only
when it is perfectly sweet that the secretions of the leaves will act
upon it.

The pitcher plant undoubtedly derives its principal nourishment from
the insects it eats. It, too--unlike most other carnivorous plants,
which, when the quantity of food with which they have to deal is in
excess of their powers of digestion, succumb to the effort and
die--appears to find it easy to devour any number of insects, small or
large, the operation being with it simply a question of time. Flies,
beetles, or even cockroaches, at the expiration of three or four days
at most, disappear, nothing being left of them save their wings and
other hard, parts of their bodies.

The _Sarracenia_ is, indeed, not only the most voracious of all known
species of carnivorous plants, but the least fastidious as to the
nature of the food upon which it feeds.--_W.C.M., Nature._

       *       *       *       *       *




WHAT IS A PLANT?


Mr. Worsley-Benison has been discussing this question in a very
interesting way, and he says in conclusion that "_physiologically_ the
most distinctive feature of plant-life is the power to manufacture
protein from less complex bodies; that of animal-life, the absence of
such power." He finds that in form, in the presence of starch, of
chlorophyl, in power of locomotion, in the presence of circulatory
organs, of the body called nitrogen, in the functions of respiration
and sensation, there are no diagnostic characters. He finds, however,
"fairly constant and well-marked distinctions" in the presence of a
cellulose coat in the plant-cell, in digestion followed by absorption,
and in the power to manufacture protein.

The _morphological_ feature of plants is this cellulose coat; of
animals, its absence; the _physiological_ peculiarity of plants, this
_manufacturing power_; of animals, the want of it. But after all the
discussion he says: "To the question, _Is this an animal or a plant?_
we must often reply, _We do not know_."--_The Microscope._

       *       *       *       *       *




CAMELLIAS.


Next to the rose, no flower* is more beautiful or more useful than the
camellia. It may readily be so managed that its natural season of
blooming shall be from October to March, thus coming in at a time when
roses can hardly be had without forcing. In every quality, with the
single exception of scent, the camellia may be pronounced the equal of
the rose. It can be used in all combinations or for all purposes for
which roses can be employed. In form and color it is probably more
perfect, and fully as brilliant. It is equally or more durable, either
on the plant or as a cut flower. It is a little dearer to buy, and
perhaps slightly more difficult to cultivate; but like most plants the
camellia has crucial periods in its life, when it needs special
treatment. That given, it may be grown with the utmost ease; that
withheld, its culture becomes precarious, or a failure. The camellia
is so hardy that it will live in the open air in many parts of Great
Britain, and herein lies a danger to many cultivators. Because it is
quite or almost hardy, they keep it almost cool. This is all very well
if the cool treatment be not carried to extremes, and persisted in all
the year round. Camellias in a dormant state will live and thrive in
any temperature above the freezing point, and will take little or no
hurt if subjected to from 3 deg.-4 deg. below it, or a temperature of 27 deg.
Fahr.

   * Transcriber's Note: Original "flour".

They will also bloom freely in a temperature of 40 deg., though 45 deg. suits
them better. Hence, during the late summer and early autumn it is
hardly possible to keep camellias too cool either out of doors or in.
They are also particularly sensitive to heat just before the
flower-buds begin to swell in late autumn or winter; a sudden or
sensible rise of temperature at that stage sends the flower-buds off
in showers. This is what too often happens, in fact, to the camellias
of amateurs. No sooner do the buds begin to show then a natural
impatience seizes the possessor's of well-budded camellias to have the
flowers opened. More warmth, a closer atmosphere, is brought to bear
upon them, and down fall the buds in showers on stage or floor--the
chief cause of this slip between the buds and the open flowers being a
rise of temperature. A close or arid atmosphere often leads to the
same results. Camellias can hardly have too free a circulation of air
or too low a temperature. Another frequent cause of buds dropping
arises from either too little or too much water at the roots. Either a
paucity or excess of water at the roots should lead to identical
results. Most amateurs overwater their camellias during their
flowering stages. Seeing so many buds expanding, they naturally rush
to the conclusion that a good deal of water must be used to fill them
to bursting point. But the opening of camellia buds is less a
manufacture than a mere development, and the strain on the plant and
drain on the roots is far less during this stage than many suppose. Of
course the opposite extreme of over-dry roots must be provided
against, else this would also cause the plants to cast off their buds.

But our object now is less to point out how buds are to be developed
into fully expanded flowers than to show how they were to be formed in
plenty, and the plants preserved in robust health year after year. One
of the simplest and surest modes of reaching this desirable end is to
adopt a system of semi-tropical treatment for two months or so after
flowering. The moment or even before the late blooms fade, the plants
should be pruned if necessary. Few plants bear the knife better than
camellias, though it is folly to cut them unless they are too tall or
too large for their quarters or have grown out of form. As a rule
healthy camellias produce sufficient or even a redundancy of shoots
without cutting back; but should they need pruning, after flowering is
the best time to perform the operation.

During the breaking of the tender leaves and the growth of the young
shoots in their first stages, the plant should be shaded from direct
sunshine, unless, indeed, they are a long way from the glass, when the
diffusion and dispersion of the rays of light tone down or break their
scorching force; few young leaves and shoots are more tender and
easily burned than camellia, and scorching not only disfigures the
plants, but also hinders the formation of fine growths and the
development of flower-buds.

The atmosphere during the early season of growth may almost touch
saturation. It must not fail to be genial, and this geniality of the
air must be kept up by the surface-sprinkling of paths, floors,
stages, walls, and the plants themselves at least twice a day.

With the pots or border well drained it is hardly possible to
overwater the roots of camellias during their period of wood-making.
The temperature may range from 50 deg. to 65 deg. during most of the period.
As the flower-buds form, and become more conspicuous, the tropical
treatment may become less and less tropical, until the camellias are
subjected to the common treatment of greenhouse or conservatory plants
in summer. Even at this early stage it is wise to attend to the
thinning of the buds. Many varieties of camellias--notably that most
useful of all varieties, the double white--will often set and swell
five or ten times more buds than it ought to be allowed to carry.
Nothing is gained, but a good deal is lost, by allowing so many embryo
flower-buds to be formed or partially developed. It is in fact far
wiser to take off the majority of the excess at the earliest possible
point, so as to concentrate the strength of the plant into those that
remain.

As it is, however, often a point of great moment to have a succession
of camellia flowers for as long a period as possible on the same
plants, buds of all sizes should be selected to remain. Fortunately,
it is found in practice that the plants, unless overweighted with
blooms, do not cast off the smaller or later buds in their efforts to
open their earlier and larger ones. With the setting, thinning, and
partial swelling of the flower-buds the semi-tropical treatment of
camellias must close; continued longer, the result would be their
blooming out of season, or more probably their not blooming at all.

The best place for camellias from the time of setting their
flower-buds to their blooming season is a vexed question, which can
hardly be said to have been settled as yet. They may either be left in
a cool greenhouse, or placed in a shaded, sheltered position in the
open air. Some of the finest camellias ever seen have been placed in
the open air from June to October. These in some cases have been stood
behind south, and in others behind west walls. Those facing the east
in their summer quarters were, on the whole, the finest, many of them
being truly magnificent plants, not a few of them having been imported
direct from Florence at a time when camellias were far less grown in
England than now.

In all cases where camellias are placed in the open air in summer,
care will be taken to place the pots on worm proof bases, and to
shield the tops from direct sunshine from 10 to 4 o'clock. If these
two points are attended to, and also shelter from high winds, it
matters little where they stand. In all cases it is well to place
camellias under glass shelter early in October, less for fear of cold
than of saturating rains causing a sodden state of the soil in the
pots.

While adverting, however, to the safety and usefulness of placing
camellias in the open air in summer, it must not be inferred that this
is essential to the successful culture; it is, in fact, far otherwise,
as the majority of the finest camellias in the country are planted out
in conservatories with immovable roofs. Many such houses are, however,
treated to special semi-tropical treatment as has been described, and
are kept as cool and open as possible after the flower-buds are fairly
set, so that the cultural and climatic conditions approximate as
closely as possible to those here indicated.

Soil and seasons of potting may be described as vexed questions in
camellia culture. As to the first, some affect pure loam, others peat
only, yet more a half and half of both, with a liberal proportion of
gritty sand, or a little smashed charcoal or bruised bones as porous
or feeding agents, or both. Most growers prefer the mixture, and as
good camellias are grown in each of its constituents, it follows
without saying that they may also be well grown in various proportions
of both.

Under rather than over potting suits the plants best, and the best
time is doubtless just before they are about to start into fresh
growth, though many good cultivators elect to shift their plants in
the late summer or autumn, that is, soon after the growth is
finishing, and the flower-buds fairly and fully set for the next
season. From all which it is obvious that the camellia is not only
among the most useful and showy, but likewise among the most
accommodating of plants.

Under good cultivation it is also one of the cleanest, though when
scab gets on it, it is difficult to get rid of it. Mealy-bugs also
occasionally make a hurried visit to camellias when making their
growth, as well as aphides. But the leaves once formed and advanced to
semi-maturity are too hard and leathery for such insects, while they
will bear scale being rubbed off them with impunity. But really
well-grown camellias, as a rule, are wholly free from insect pests,
and their clean, dark, glossy leaves are only of secondary beauty to
their brilliant, exquisitely formed, and many sized flowers.--_D.T.,
The Gardeners' Chronicle._

       *       *       *       *       *




ARISAEMA FIMBRIATUM.

_Mast.; sp. nov._


[Illustration: ARISAEMA FIMBRIATUM: LEAF, SPATHE, AND FLORAL DETAILS.]

Some few years since we had occasion to figure some very remarkable
Himalayan species of this genus, in which the end of the spadix was
prolonged into a very long, thread-like appendage thrown over the
leaves of the plant or of its neighbors, and ultimately reaching the
ground, and thus, it is presumed, affording ants and other insects
means of access to the flowers, and consequent fertilization. These
species were grown by Mr. Elwes, and exhibited by him before the
Scientific Committee. The present species is of somewhat similar
character, but is, we believe, new alike to gardens and to science. We
met with it in the course of the autumn in the nursery of Messrs.
Sander, at St. Alban's; but learn that it has since passed into the
hands of Mr. W. Bull, of Chelsea. It was imported accidentally with
orchids, probably from the Philippine Islands. It belongs to Engler's
section, trisecta, having two stalked leaves, each deeply divided into
three ovate acute glabrous segments. The petioles are long, pale
purplish, rose-colored, sprinkled with small purplish spots. The
spathes are oblong acute or acuminate, convolute at the base,
brownish-purple, striped longitudinally with narrow whitish bands. The
spadix is cylindrical, slender, terminating in along, whip-like
extremity, much longer than the spathe. The flowers have the
arrangement and structure common to the genus, the females being
crowded at the base of the spadix, the males immediately above them,
and these passing gradually into fleshy incurved processes, which in
their turn pass gradually into long, slender, purplish threads,
covering the whole of the free end of the spadix.--_M.T.M., in The
Gardeness' Chronicle._

       *       *       *       *       *




STRIKING A LIGHT.


In the new edition of Mason's "Burma" we read that among other uses to
which the bamboo is applied, not the least useful is that of producing
fire by friction. For this purpose a joint of thoroughly dry bamboo is
selected, about 11/2 inches in diameter, and this joint is then split in
halves. A ball is now prepared by scraping off shavings from a
perfectly dry bamboo, and this ball being placed on some firm support,
as a fallen log or piece of rock, one of the above halves is held by
its ends firmly down on it, so that the ball of soft fiber is pressed
with some force against its inner or concave surface. Another man now
takes a piece of bamboo a foot long or less, and shaped with a blunt
edge, something like a paper knife, and commences a sawing motion
backward and forward across the horizontal piece of bamboo, and just
over the spot where the ball of soft fiber is held. The motion is slow
at first, and by degrees a groove is formed, which soon deepens as the
motion increases in quickness. Soon smoke arises, and the motion is
now made as rapid as possible, and by the time the bamboo is cut
through not only smoke but sparks are seen, which soon ignite the
materials of which the ball beneath is composed. The first tender
spark is now carefully blown, and when well alight the ball is
withdrawn, and leaves and other inflammable materials heaped over it,
and a fire secured. This is the only method that I am aware of for
procuring fire by friction in Burma, but on the hills and out of the
way parts, that philosophical toy, the "pyrophorus," is still in use.
This consists[1] of a short joint of a thick woody bamboo, neatly cut,
which forms a cylinder. At the bottom of this a bit of tinder is
placed, and a tightly-fitting piston inserted composed of some hard
wood. The tube being now held in one hand, or firmly supported, the
piston is driven violently down on the tinder by a smart blow from the
hand, with the result of igniting the tinder beneath.

   [Footnote 1: It is also made of a solid cylinder of buffalo's
   horn, with a central hollow of three-sixteenths of an inch in
   diameter and three inches deep burnt into it. The piston, which
   fits very tightly in it, is made of iron-wood or some wood
   equally hard.]

Another method of obtaining fire by friction from bamboos is thus
described by Captain T.H. Lewin ("Hill Tracts of Chittagong, and the
Dwellers Therein", Calcutta, 1869, p. 83), as practiced in the
Chittagong Hills. The Tipporahs make use of an ingenious device to
obtain fire; they take a piece of dry bamboo, about a foot long, split
it in half, and on its outer round surface cut a nick, or notch, about
an eighth of an inch broad, circling round the semi-circumference of
the bamboo, shallow toward the edges, but deepening in the center
until a minute slit of about a line in breadth pierces the inner
surface of the bamboo fire-stick. Then a flexible strip of bamboo is
taken, about 11/2 feet long and an eighth of an inch in breadth, to fit
the circling notch, or groove, in the fire-stick. This slip or band is
rubbed with fine dry sand, and then passed round the fire-stick, on
which the operator stands, a foot on either end. Then the slip,
grasped firmly, an end in each hand, is pulled steadily back and
forth, increasing gradually in pressure and velocity as the smoke
comes. By the time the fire-band snaps with the friction there ought
to appear through the slit in the fire-stick some incandescent dust,
and this placed, smouldering as it is, in a nest of dry bamboo
shavings, can be gently blown into a flame.--_The Gardeners'
Chronicle._

       *       *       *       *       *




EXPERIMENTS IN MEMORY.


When we read how one mediaeval saint stood erect in his cell for a week
without sleep or food, merely chewing a plantain-leaf out of humility,
so as not to be too perfect; how another remained all night up to his
neck in a pond that was freezing over; and how others still performed
for the glory of God feats no less tasking to their energies, we are
inclined to think, that, with the gods of yore, the men, too, have
departed, and that the earth is handed over to a race whose will has
become as feeble as its faith. But we ought not to yield to these
instigations, by which the evil one tempts us to disparage our own
generation. The gods have somewhat changed their shape, 'tis true, and
the men their minds; but both are still alive and vigorous as ever for
an eye that can look under superficial disguises. The human energy no
longer freezes itself in fish-ponds, and starves itself in cells; but
near the north pole, in central Africa, on Alpine "couloirs," and
especially in what are nowadays called "psycho-physical laboratories,"
it maybe found as invincible as ever, and ready for every fresh
demand. To most people a north pole expedition would be an easy task
compared with those ineffably tedious measurements of simple mental
processes of which Ernst Heinrich Weber set the fashion some forty
years ago, and the necessity of extending which in every possible
direction becomes more and more apparent to students of the mind.
Think of making forty thousand estimates of which is the heavier of
two weights, or seventy thousand answers as to whether your skin is
touched at two points or at one, and then tabulating and
mathematically discussing your results! Insight is to be gained at no
less price than this. The new sort of study of the mind bears the same
relation to the older psychology that the microscopic anatomy of the
body does to the anatomy of its visible form, and the one will
undoubtedly be as fruitful and as indispensable as the other.

Dr. Ebbinghaus[1] makes an original addition to heroic psychological
literature in the little work whose title we have given. For more than
two years he has apparently spent a considerable time each day in
committing to memory sets of meaningless syllables, and trying to
trace numerically the laws according to which they were retained or
forgotten. Most of his results, we are sorry to say, add nothing to
our gross experience of the matter. Here, as in the case of the
saints, heroism seems to be its own reward. But the incidental results
are usually the most pregnant in this department; and two of those
which Dr. Ebbinghaus has reached seems to us to amply justify his
pains. The first is, that, in _forgetting_ such things as these lists
of syllables, the loss goes on very much more rapidly at first than
later on. He measured the loss by the number of seconds required to
_relearn_ the list after it had been once learned. Roughly speaking,
if it took a thousand seconds to learn the list, and five hundred to
relearn it, the loss between the two learnings would have been
one-half. Measured in this way, full half of the forgetting seems to
occur within the first half-hour, while only four-fifths is forgotten
at the end of a month. The nature of this result might have been
anticipated, but hardly its numerical proportions.

   [Footnote 1: "Ueber das Gedaechtniss. Untersuchungen zur
   experimentellen Psychologie." Von Herm.
   Ebbinghaus. Leipzig: Duncker u. Humblot, 1885. 10+169 pp. 8vo.]

The other important result relates to the question whether ideas are
recalled only by those that previously came immediately before them,
or whether an idea can possibly recall another idea, with which it was
never in _immediate_ contact, without passing through the intermediate
mental links. The question is of theoretic importance with regard to
the way in which the process of "association of ideas" must be
conceived; and Dr. Ebbinghaus' attempt is as successful as it is
original, in bringing two views, which seem at first sight
inaccessible to proof, to a direct practical test, and giving the
victory to one of them. His experiments conclusively show that an idea
is not only "associated" directly with the one that follows it, and
with the rest _through that_, but that it is _directly_ associated
with _all_ that are near it, though in unequal degrees. He first
measured the time needed to impress on the memory certain lists of
syllables, and then the time needed to impress lists of the same
syllables with gaps between them. Thus, representing the syllables by
numbers, if the first list was 1, 2, 3, 4 ... 13, 14, 15, 16, the
second would be 1, 3, 5 ... 15, 2, 4, 6 ... 16, and so forth, with
many variations.

Now, if 1 and 3 in the first list were learned in that order merely by
1 calling up 2, and by 2 calling up 3, leaving out the 2 ought to
leave 1 and 3 with no tie in the mind; and the second list ought to
take as much time in the learning as if the first list had never been
heard of. If, on the other hand, 1 has a _direct_ influence on 3 as
well as on 2, that influence should be exerted even when 2 is dropped
out; and a person familiar with the first list ought to learn the
second one more rapidly than otherwise he could. This latter case is
what actually occurs; and Dr. Ebbinghaus has found that syllables
originally separated by as many as seven intermediaries still reveal,
by the increased rapidity with which they are learned in order, the
strength of the tie that the original learning established between
them, over the heads, so to speak, of all the rest. It may be that
this particular series of experiments is the entering wedge of a new
method of incalculable reach in such questions. The future alone can
show. Meanwhile, when we add to Dr. Ebbinghaus' "heroism" in the
pursuit of true averages, his high critical acumen, his modest tone,
and his polished style, it will be seen that we have a new-comer in
psychology from whom the best may be expected.--_W.J., Science._

       *       *       *       *       *




SINKING OF THE QUIEVRECHAIN WORKING SHAFT.


The sinking of mine shafts in certain Belgian and French basins, where
the coal deposit is covered with thick strata of watery earth, has
from all times been considered as the most troublesome and delicate,
and often the most difficult operation, of the miner's art. Of the few
modern processes that have been employed for this purpose, that of
Messrs. Kind and Chaudron has been found most satisfactory, although
it leaves much to be desired where it is a question of traversing
moving sand. An interesting modification of this well-known process
has recently been described by Mr. E. Chavatte, in the Bulletin de la
Societe Industrielle du Nord de la France. Two years ago the author
had to sink a working shaft at Quievrechain, 111 feet of which was to
traverse a mass of moving and flowing sand, inconsistent earth,
gravel, and marls, and proceeded as follows:

He first put down two beams, A B (Pl. 1, Figs. 2, 3, and 9), each 82
feet in length and of 20x20 inch section in the center, and upon these
placed two others, E F, of 16x16 inch section. Beneath the two first
were inserted six joists, _c c c c c c_, about 82 feet in length and
of 14 or 16 inch section in the center. Finally these were
strengthened at their extremities with two others, _d d_, about 82
feet in length. All these timbers, having been connected by tie bands
and bolts, constituted a rigid structure that covered a surface of
nearly seven hundred square yards.

From the beams, A B and E F, there was suspended a red fir frame by
means of thirty-four iron rods.

Upon this frame, which was entirely immersed in the moving sand, there
was established brick masonry (Figs. 1, 2, and 3). As the ends of the
timbers entered the latter, and were connected by 11/2 inch bolts, they
concurred in making the entire affair perfectly solid. The frame, K K,
was provided with an oaken ring, which was affixed to it with bolts.

After this, a cast iron tubbing, having a cutting edge, and being
composed of rings 3.28 feet wide and made of six segments, was
lowered. This tubbing was perfectly tight, all the surfaces of the
joints having been made even and provided with strips of lead
one-tenth of an inch thick. It weighed 4,000 pounds to the running
foot.

[Illustration: FIG. 1.--Section through A B. FIG. 2.--Plan. FIG.
3.--Section through C D. FIG. 5.--Section through E F of Fig. 4. FIGS.
6 AND 7.--Work Prepared and finished. FIG. 10.--Section through A B
and C D of Fig. 12. FIGS. 11 6 AND 12.--Arrangement of jack-screw.
FIG. 13.--Section through A B and C D of Fig. 11.

               PLATE I.--SINKING A MINE SHAFT.]

It was first raised to a height of fifteen feet, so as to cause it to
enter the sand by virtue of its own gravity. It thus penetrated to a
depth of about twenty inches. After this the workmen were ordered to
man the windlasses and hoist out some of the sand. This caused the
tubbing to descend about eight inches more, when it came to a
standstill. It was now loaded with 17,000 pounds of pig iron, but in
vain, for it refused to budge. Mr. Chavatte therefore had recourse to
a dredge with vertical axis, constructed as follows:

Upon a square axis, A B (Pl. 2, Figs. 1, 2, and 3), provided with
double cross braces, C D, and strengthened by diagonals, were riveted,
by their upper extremities, two cheeks, G H, whose lower extremities
held the steel plates, I J I' J', which, in turn, were fastened to the
axis, A B, by their other extremities. These plates were so inclined
as to scrape the surface of the ground over which they were moved.
They each carried two bags made of coarse canvas and strengthened by
five strong leather straps (Figs. 2 and 4). To the steel plates were
riveted two plates of iron containing numerous apertures, through
which passed leather straps designed for fastening thereto the lower
part of the mouth of the bags. That portion of the mouth of the latter
that was to remain open was fastened in the same way to two other
plates, X Y, X¹ Y¹ (Fig. 1), held between the lower cross-braces.

When the apparatus was revolved, the plates scraped the earth to be
removed, and descended in measure as the latter entered the bags.
These bags, when full, were hooked, by means of the five rings which
they carried, to the device shown in Fig. 8 (Pl. 2), and raised to the
surface and emptied into cars.

The dredge was set in motion by four oak levers (Figs. 5 and 6). Two
of these were manned by workmen stationed upon the surface flooring,
and the other two by workmen upon the flooring in the tubbing. The
axis was elongated, in measure as the apparatus descended, by rods of
the same dimensions fastened together by cast iron sleeves and bolts
(Fig. 7).

The steel plates were not capable of acting alone, even in cases where
they operated in pure moving sand containing no pebbles, for the sand
was too compact to be easily scraped up by the steel, and so it had to
be previously divided. For this purpose Mr. Chavatte used rakes which
were in form exactly like those of the extirpators, U and V, of Figs.
1, 2, and 3, of Pl. 2, except that the dividers carried teeth that
were not so strong as those of the extirpators, and that were set
closer together. These rakes were let down and drawn up at will. They
were maneuvered as follows:

The dredge descended with the extirpators pointing upward. When their
heads reached the level of the upper floor, the tools were removed.
Then the dredge was raised again. In this way the extirpators lay upon
the floor, and, if the lifting was continued, they placed themselves
in their working position, in which they were fixed by the bolts A" B"
C" (Fig. 1). After this, the apparatus was let down and revolved. The
rakes divided the earth, the scrapers collected it, and the bags
pocketed it.

The great difficulty was to cause the tubbing to descend vertically,
and also to overcome the enormous lateral pressure exerted upon it by
the earth that was being traversed. Water put into the shaft helped
somewhat, but the great stress to be exerted had to be effected by
means of powerful jack screws. These were placed directly upon the
tubbing, and bore against strong beams whose extremities were inserted
into the masonry.

As a usual thing it is not easy to use more than four or six such
jacks, since the number of beams that can be employed is limited,
owing to the danger of obstructing the mouth of the shaft. Yet twelve
were used by Mr. Chavatte, and this number might have been doubled had
it been necessary. As we have seen, the frame, K K (Pl. 1, Fig. 3),
was provided with an oak circle traversed by 32 bolts. The length of
these latter was two inches and a quarter longer than they needed to
have been, or they were provided with wooden collars of that
thickness. Later on, these collars were replaced with iron bars that
held the wood against which the jacks bore in order to press the
tubbing downward (Pl. 1, Figs. 10, 11, 12, and 13).

Mr. Chavatte's great anxiety was to know whether he should succeed in
causing the first section of tubbing to traverse the four feet of
gravel; for in case it did not pass, he would be obliged to employ a
second section of smaller diameter, thus increasing the expense. He
was persuaded that the coarse gravel remaining in the side of the
shaft would greatly retard the descent of the tubbing. So he had
decided to remove such obstructions at the proper moment through
divers or a diving bell. Then an idea occurred to him that dispensed
with all that trouble, and allowed him to continue with the first
section. This was to place upon the dredge two claw-bars, T (Pl. 2,
Fig. 3), which effected the operation of widening with wonderful ease.
To do this it was only necessary to turn up the bags, and revolve the
apparatus during its descent. The claw at the extremity of the bar
pulled out everything within its reach, and thus made an absolutely
free passage for the tubbing.

The sands and gravels were passed by means of a single section of
tubbing 31 feet in length, which was not stopped until it had
penetrated a stratum of white chalk to a depth of two yards. This
chalk had no consistency, although it contained thin plates of quite
large dimensions. These were cut, as if with a punch, by means of the
teeth of the extirpator.

It now remains to say a few words concerning the sinking of the shaft,
which, after the operation of the dredge, was continued by the process
called "natural level" The work was not easy until a depth of 111 feet
had been reached. Up to this point it had been necessary to proceed
with great prudence, and retain the shifting earth by means of four
iron plate tubes weighing 54 tons. Before finding a means of widening
the work already done by the dredge, Mr. Chavatte was certain that he
would have to use two sections of tubbing, and so had given the first
section a diameter of 161/2 feet. He could then greatly reduce the
diameter, and bring it to 153/4 feet as soon as the ground auger was
used.

After two yards of soil had been removed from beneath the edge of the
tubbing, the earth began to give way. Seeing this, Mr. Chavatte let
down a tube 13 feet in length and 15.4 in diameter. The exterior of
this was provided with 12 oak guides, which sliding over the surface
of the tubbing had the effect of causing the tube to descend
vertically. And this was necessary, because this tube had to be driven
down every time an excavation of half a yard had been made.

Afterward, a diameter of 15.35 feet was proceeded with, and the small
central shaft of 41/4 feet diameter was begun. This latter had not as
yet been sunk, for fear of causing a fall of the earth.

Next, the earth was excavated to a depth of 8.2 feet, and a tube 16.4
feet in length was inserted; then a further excavation of 8.2 feet was
made, and the tube driven home.

After this an excavation of 261/4 feet was made, and a tube of the same
length and 141/2 feet in diameter was driven down. Finally, the shifting
soil was finished with a fourth tube 191/2 feet in length and 14 feet in
diameter.

A depth of 111 feet had now been reached, and the material encountered
was solid white chalk. From this point the work proceeded with a
diameter of 13.9 feet to a depth of 450 feet. The small shaft had been
sunk directly to a depth of 475 feet. At 450 feet the diameter was
diminished by three inches. Then an advance of a foot was made, and
the diameter reduced by one and a half inch.

The reason for this reduction in the diameter and change in the mode
of deepening was as follows:

The Chaudron moss-box, when it chances to reach its seat intact, and
can consequently operate well, undoubtedly makes a good wedging. But
how many times does it not happen that it gets injured before reaching
its destination? Besides, as it often rests upon earth that has caved
in upon its seat during the descent of the tubbing, it gets askew, and
later on has to be raised on one side by means of jacks or other
apparatus. Under such circumstances, Mr. Chavatte considered this
moss-box as more detrimental than useful, and not at all
indispensable, and so substituted beton for it, as had previously been
done by Mr. Bourg, director of the Bois-du-Luc coal mines.

[Illustration: FIGS. 1, 2, 3, 6 AND 4.--Details of dredge. FIGS. 5 6
AND 6.--Details of maneuvering lever. FIG. 7.--Mode of lengthening the
axis of the dredge. FIG. 8.--Hooks for lifting the dredge bags. FIG.
9.--Arrangement of valves in the beton box. FIG. 10.--Device for
centering the tubbing.

               PLATE II.]

This engineer likewise suppressed the balancing column, which is often
a source of trouble in the descent of the tubbing, and forced his
tubbing to center itself with the shaft through a guide with four
branches riveted under the false bottom that entered the small shaft
(Pl. 2, Fig. 10). Mr. Bourg so managed that there remained an empty
space of ten inches to fill in with beton. Mr. Chavatte had at first
intended to proceed in the same way, but the two last tubbings, upon
which he had not counted, forced him to reduce the space to 53/4 inches.
Under such circumstances it was not prudent to employ the same means
for guiding the base of the tubbing, because, if the central shaft had
not exactly the same center as the large one, there would have been
danger of throwing the tubbing sideways and causing it to leak. Seeing
which, Mr. Chavatte strengthened the lower part of the base ring and
placed it upon another ring tapering downward, and 271/2 inches in
height (Pl. 1, Fig. 5). The object of this lower ring was to force the
tubbing to remain concentric with the shaft, to form a tight joint
with its upper conical portion, and to form a joint upon the seat with
its lower flange, so as to prevent the beton from flowing into the
small shaft.

After the shaft was pumped out, digging by hand was begun with a
diameter of 12 feet. After descending 20 inches an 8x10 inch curb was
laid, in order to consolidate the earth and prevent any movement of
the tubbing. Then the excavating was continued to a depth of 311/2
inches, and with a diameter of 93/4 feet. At this point another curb was
put in for consolidating the earth. Finally, the bottom was widened
out as shown in Fig. 7, so that three basal wedged curbs could be put
in. This done, the false tubbing was put in place; and finally, when
proceeding upward, the last ring composed of twelve pieces was
reached, the earth was excavated and at once replaced with a collar
composed of twelve pieces of oak tightened up by oak wedges. Each of
these pieces was cemented separately and in measure as they were
assembled.

Through motive of economy no masonry was placed under the base of the
three wedged curbs. In fact, by replacing this with a wedged curb of
wood traversed by six bolts designed to fix the cast iron curb
immediately above, Mr. Chavatte obtained a third curb that he would
have had to have made of cast iron.

       *       *       *       *       *




ON THE ELEMENTARY PRINCIPLES OF THE GAS-ENGINE.[1]

   [Footnote 1: A paper read before the Gas Institute, Manchester,
   June, 1885.]

By DENNY LANE, of Cork.


Among the most useful inventions of the latter half of the nineteenth
century the gas-engine holds a prominent place. While its development
has not been so brilliant or so startling as that which we can note in
the employment of electricity, it holds, among the applications of
heat, the most important place of any invention made within that
period. Even amid the contrivances by which, in recent times, the
other forces of nature have been subdued to the uses of man, there are
only a few which rival the gas-engine in practical importance. With
regard to the steam-engine itself, it is remarkable how little that is
new has really been invented since the time of Watt and Woulfe. In the
specifications of the former can be shown completely delineated, or
fully foreshadowed, nearly every essential condition of the economy
and efficiency attained in our own days; and it is only by a gradual
"survival of the fittest" of the many contrivances which were made to
carry out his broad ideas that the steam-engine of the present has
attained its great economy.

It is but within the last fifty years that the laws of the relation
between the different physical forces were first enunciated by Justice
Grove, and confirmed by the classical researches of Dr. Joule--the one
a lawyer, working hard at his profession, the other a man of business
engaged in manufacture. Both are still living among us; the latter
having withdrawn from business, while the former is a Judge of the
High Court of Justice. I always regret that the claims of his
profession have weaned Justice Grove from science; for, while it may
be possible to find in the ranks of the Bar many who might worthily
occupy his place on the Bench, it would be hard to find among men of
science any with as wide-reaching and practical philosophy as that
which he owns. The chemist demonstrated long since that it was
impossible for man to create or destroy a single particle of
ponderable matter; but it remained for our own time to prove that it
was equally impossible to create or destroy any of the energy which
existed in nature as heat, mechanical power, electricity, or chemical
affinity. All that it is in the power of man to do is to convert one
of these forms into another. This, perhaps the greatest of all
scientific discoveries since the time of Newton, was first, I believe,
enunciated in 1842 by Grove, in a lecture given at the London
Institution; and it was experimentally proved by the researches of
Joule, described in a paper which he read at the meeting of the
British Association which was held at Cork--my native city--in 1843.
My friend Dr. Sullivan, now President of Queen's College, Cork, and I
myself had the privilege of being two of a select audience of half a
dozen people, who alone took sufficient interest in the subject to
hear for the first time developed the experimental proof of the theory
which welds into one coherent system the whole physical forces of the
universe, and enables one of these to be measured by another. One
branch of the "correlation of physical forces," as it was termed by
Grove, was the relation between mechanical power and heat, and the
convertibility of each into the other, which, under the name of
"Thermodynamics," has become one of the most important branches of
practical science.

Joule's first experiments clearly proved that each of these forms of
energy was convertible into the other; but some discrepancies arose in
determining the exact equivalent of each. His subsequent researches,
however, clearly demonstrated the true relation between both. Taking
as the unit of heat the amount which would be necessary to raise 1 lb.
of water 1 deg. of Fahrenheit's scale (now called "the English thermal
unit"), he proved that this unit was equivalent to the mechanical
power which would be required to raise 772 lb. 1 foot, or to raise 1
lb. 772 ft. perpendicularly against the force of gravity. The
heat-unit--the pound-degree--which I will distinguish by the Greek
letter [theta], is a compound unit of mass and temperature; the
second--the foot-pound = f.p.--a compound unit of mass and space. This
equation, called "Joule's equivalent," or 1 thermal unit = 772
foot-pounds, is the foundation and the corner-stone of thermodynamics.

It is essential to understand the meaning of this equation. It
expresses the maximum effect of the given cause, viz., that if _all_
the heat were converted into power, or _all_ the power were converted
into heat, 1 thermal unit would produce 772 foot-pounds, or 772
foot-pounds would raise 1 lb. of water 1 deg. Fahr. But there is never a
complete conversion of any form of energy. Common solid coal may be
partly converted into gases in a retort; but some of the carbon
remains unchanged, and more is dissipated but not lost. In the same
way, if I take five sovereigns to Paris and convert them into francs,
and return to London and convert the francs into shillings, I shall
not have 100 shillings, but only perhaps 95 shillings. But the five
shillings have not been lost; three of them remain in the French
_change de monnaies_, and two of them in the English exchange office.
I may have forfeited something, but the world has forfeited nothing.
There remains in it exactly the same number of sovereigns, francs, and
shillings as there was before I set out on my travels. Nothing has
been lost, but some of my money has been "dissipated;" and the
analogous case, "the dissipation of energy," has formed the subject of
more than one learned essay.

Before the invention of the steam-engine, the only powers employed in
mechanics were those of wind and water mills, and animal power. In the
first two, no conversion of one force into another took place; they
were mere kinematic devices for employing the mechanical force already
existing in the gale of wind and the head of water. With regard to the
power developed by man and other animals, we had in them examples of
most efficient heat-engines, converting into power a large percentage
of the fuel burnt in the lungs. But animal power is small in amount,
and it is expensive for two reasons--first, because the agents require
long intervals of rest, during which they still burn fuel; and next,
because the fuel they require is very expensive. A pound of bread or
beef, or oats or beans, costs a great deal more than a pound of coal;
while it does not, by its combustion, generate nearly so much heat.
The steam-engine, therefore, took the place of animal power, and for a
long time stood alone; and nearly all the motive power derived from
heat is still produced by the mechanism which Watt brought to such
great efficiency in so short a time.

Now the practical question for all designers and employers of
heat-engines is to determine how the greatest quantity of motive force
can be developed from the heat evolved from a given kind of fuel; and
coal being the cheapest of all, we will see what are the results
obtainable from it by the steam-engine. In this we have three
efficiencies to consider--those of the furnace, the boiler, and the
cylinder.

First, with respect to the furnace. The object is to combine the
carbon and the hydrogen of the coal with a sufficient quantity of the
oxygen of the air to effect complete combustion into carbonic acid and
water. In order to do this, we have to use a quantity of air much
larger than is theoretically necessary, and also to heat an amount of
inert nitrogen five times greater than the necessary oxygen; and we
are therefore obliged to create a draught which carries away to the
chimney a considerable portion of the heat developed. The combustion,
moreover, is never perfect; and some heat is lost by conduction and
radiation. The principal loss is by hot gases escaping from the flues
to the chimney. Even with well-set boilers, the temperature in the
chimney varies from 400 deg. to 600 deg. Fahr. Taking the mean of 500 deg., this
would represent a large proportion of the total heat, even if the
combustion were perfect; for, as a general rule, the supply of air to
a furnace is double that which is theoretically necessary. For our
present purpose, it will be sufficient to see how much the whole loss
is, without dividing it under the several heads of "imperfect
combustion," "radiation," and "convection," by the heated gases
passing to the chimney.

With a very good boiler and furnace each pound of coal evaporates 10
pounds of water from 62 deg. Fahr., changing it into steam of 65 lb.
pressure at a temperature of 312 deg., or 250 deg. above that of the water
from which it is generated. Besides these 250 deg., each pound of steam
contains 894 units of latent heat, or 1,144 units in all. A very good
condensing engine will work with 2.2 lb. of coal and 22 lb. of steam
per horse power per hour. Now. 1 lb. of good coal will, by its
combustion, produce 14,000 heat-units; and the 2.2 lb. of coal
multiplied by 14,000 represent 30,800[theta]. Of these we find in the
boiler 22 x 1,144, or 25,168 units, or about 811/2 per cent., of the
whole heat of combustion; so that the difference (5,632 units, or 181/2
per cent.) has been lost by imperfect combustion, radiation, or
convection. The water required for condensing this quantity of steam
is 550 lb.; and, taking the temperature in the hot well as 102 deg., 550
lb. have been raised 40 deg. from 62 deg.. Thus we account for 550 x 40 =
22,000, or (say) 711/2 per cent. still remaining as heat. If we add this
711/2 per cent. to 181/2 per cent. we have 90 per cent., and there remain
only 10 per cent. of the heat that can possibly have been converted
into power. But some of this has been lost by radiation from
steam-pipes, cylinder, etc. Allowing but 1 per cent. for this, we have
only 9 per cent. as the efficiency of a really good condensing engine.
This estimate agrees very closely with the actual result; for the 2.2
lb. of coal would develop 30,800[theta]; and this, multiplied by
Joule's equivalent, amounts to nearly 24 millions of foot-pounds. As 1
horse power is a little less than 2 million foot-pounds per hour, only
one-twelfth, or a little more than 8 per cent. of the total heat is
converted; so that whether we look at the total quantity of heat which
we show unconverted, or the total heat converted, we find that each
supplements and corroborates the other. If we take the efficiency of
the engine alone, without considering the loss caused by the boiler,
we find that the 25,168[theta] which entered the boiler should have
given 19,429,696 foot-pounds; so that the 2 millions given by the
engine represent about 10 per cent. of the heat which has left the
boiler. The foregoing figures refer to large stationary or marine
engines, with first-rate boilers. When, however, we come to
high-pressure engines of the best type, the consumption of coal is
twice as much; and for those of any ordinary type it is usual to
calculate 1 cubic foot, or 621/2 lb., of water evaporated per horse
power. This would reduce the efficiency to about 6 per cent. for the
best, and 3 per cent. for the ordinary non-condensing engines; and if
to this we add the inefficiency of some boilers, it is certain that
many small engines do not convert into power more than 2 per cent. of
the potential energy contained in the coal.

At one time the steam-engine was threatened with serious rivalry by
the hot-air engine. About the year 1816 the Rev. Mr. Stirling, a
Scotch clergyman, invented one which a member of this Institute (Mr.
George Anderson) remembers to have seen still at work at Dundee. The
principle of it was that a quantity of air under pressure was moved by
a mass, called a "displacer," from the cold to the hot end of a large
vessel which was heated by a fire beneath and cooled by a current of
water above. The same air was alternately heated and cooled, expanded
and contracted; and by the difference of pressure moved the piston in
a working cylinder. In this arrangement the furnace was inefficient.
As only a small portion of heat reached the compressed air, the loss
by radiation was very great, and the wear and tear exceedingly heavy.
This system, with some modifications, was revived by Rankine,
Ericsson, Laubereau, Ryder, Buckett, and Bailey. Siemens employed a
similar system, only substituting steam for air. Another system,
originally proposed by Sir George Cayley, consisted in compressing by
a pump cold air which was subsequently passed partly through a
furnace, and, expanding, moved a larger piston at the same pressure;
and the difference of the areas of the pistons multiplied by the
pressure common to both represented the indicated power. This
principle was subsequently developed by a very able mechanic, Mr.
Wenham; but his engine never came much into favor. The only hot-air
engines at present in use are Ryder's, Buckett's, and Bailey's,
employed to a limited extent for small powers. I have not said
anything of the thermal principles involved in the construction of
these engines, as they are precisely the same as those affecting the
subject of the present paper.

Before explaining the principle upon which the gas-engine and every
other hot-air engine depends, I shall remind you of a few data with
which most of you are already familiar. The volume of every gas
increases with the temperature; and this increase was the basis of the
air thermometer--the first ever used. It is to be regretted that it
was not the foundation of all others; for it is based on a physical
principle universally applicable. Although the volume increases with
the temperature, it does not increase in proportion to the degrees of
any ordinary scale, but much more slowly. Now, if to each of the terms
of an arithmetical series we add the same number, the new series so
formed increases or decreases more slowly than the original; and it
was discovered that, by adding 461 to the degrees of Fahrenheit's
scale, the new scale so formed represented exactly the increment of
volume caused by increase of temperature. This scale, proposed by Sir
W. Thomson in 1848, is called the "scale of absolute temperature." Its
zero, called the "absolute zero," is 461 deg. below the zero of
Fahrenheit, or 493 deg. below the freezing point of water; and the degree
of heat measured by it is termed the "absolute temperature." It is
often convenient to refer to 39 deg. Fahr. (which happens to be the point
at which water attains its maximum density), as this is the same as
500 deg. absolute; for, counting from this datum level, a volume of air
expands exactly 1 per cent. for 5 deg., and would be doubled at 1,000 deg.
absolute, or 539 deg. Fahr.

Whenever any body is compressed, its specific heat is diminished; and
the surplus portion is, as it were, pushed out of the body--appearing
as sensible heat. And whenever any body is expanded, its specific heat
is increased; and the additional quantity of heat requisite is, as it
were, sucked in from surrounding bodies--so producing cold. This
action may be compared to that of a wet sponge from which, when
compressed, a portion of the water is forced out, and when the sponge
is allowed to expand, the water is drawn back. This effect is
manifested by the increase of temperature in air-compressing machines,
and the cold produced by allowing or forcing air to expand in
air-cooling machines. At 39 deg. Fahr., 1 lb. of air measures 121/2 cubic
feet. Let us suppose that 1 lb. of air at 39 deg. Fahr. = 500 deg. absolute,
is contained in a non-conducting cylinder of 1 foot area and 121/2 feet
deep under a counterpoised piston. The pressure of the atmosphere on
the piston = 144 square inches x 14.7 lb., or 2,116 lb. If the air be
now heated up to 539 deg. Fahr. = 1,000 deg. absolute, and at the same time
the piston is not allowed to move, the pressure is doubled; and when
the piston is released, it would rise 121/2 feet, provided that the
temperature remained constant, and the indicator would describe a
hyperbolic curve (called an "isothermal") because the temperature
would have remained equal throughout. But, in fact, the temperature is
lowered, because expansion has taken place, and the indicator curve
which would then be described is called an "adiabatic curve," which is
more inclined to the horizontal line when the volumes are represented
by horizontal and the pressures by vertical co-ordinates. In this case
it is supposed that there is no conduction or transmission (diabasis)
of heat through the sides of the containing vessel. If, however, an
_additional_ quantity of heat be communicated to the air, so as to
maintain the temperature at 1,000 deg. absolute, the piston will rise
until it is 121/2 feet above its original position, and the indicator
will describe an isothermal curve. Now mark the difference. When the
piston was fixed, only a heating effect resulted; but when the piston
moved up 121/2 feet, not only a heating but a mechanical, in fact, a
thermodynamic, effect was produced, for the weight of the atmosphere
(2,116 lb.) was lifted 121/2 feet = 26,450 foot-pounds.

The specific heat of air at constant pressure has been proved by the
experiments of Regnault to be 0.2378, or something less than
one-fourth of that of water--a result arrived at by Rankine from
totally different data. In the case we have taken, there have been
expended 500 x 0.2378, or (say) 118.9[theta] to produce 26,450 f.p.
Each unit has therefore produced (26,450 / 118.0) = 222.5 f.p.,
instead of 772 f.p., which would have been rendered if every unit had
been converted into power. We therefore conclude that (222.5 / 772) = 29
per cent. of the total heat has been converted. The residue, or 71 per
cent., remains unchanged as heat, and may be partly saved by a
regenerator, or applied to other purposes for which a moderate heat is
required.

The quantity of heat necessary to raise the heat of air at a constant
volume is only 71 per cent. of that required to raise to the same
temperature the same weight of air under constant pressure. This is
exactly the result which Laplace arrived at from observations on the
velocity of sound, and may be stated thus--

                                            Specific        Foot-   Per
                                              heat.        pounds. cent.

Kp = 1 lb. of air at constant pressure       0.2378 x 772 = 183.5 = 100
Kv = 1 lb. of air at constant volume         0.1688 x 772 = 130.3 =  71
                                             ------   ---   -----   ---
Difference, being heat converted into power  0.0690 x 772 =  53.2 =  29


Or, in a hot-air engine without regeneration, the maximum effect of 1
lb. of air heated 1 deg. Fahr. would be 53.2 f.p. The quantity of heat
Ky necessary to heat air under constant volume is to Kv, or that
necessary to heat it under constant pressure, as 71:100, or as
1:1.408, or very nearly as 1:SQRT(2)--a result which was arrived
at by Masson from theoretical considerations. The 71 per cent.
escaping as heat may be utilized in place of other fuel; and with the
first hot-air engine I ever saw, it was employed for drying blocks of
wood. In the same way, the unconverted heat of the exhaust steam from
a high-pressure engine, or the heated gases and water passing away
from a gas-engine, may be employed.

[Illustration]

We are now in a position to judge what is the practical efficiency of
the gas-engine. Some years since, in a letter which I addressed to
_Engineering_, and which also appeared in the _Journal of Gas
Lighting_,[2] I showed (I believe for the first time) that, in the
Otto-Crossley engine, 18 per cent. of the total heat was converted
into power, as against the 8 per cent. given by a very good
steam-engine. About the end of 1883 a very elaborate essay, by M.
Witz, appeared in the _Annales de Chimie et de Physique_, reporting
experiments on a similar engine, which gave an efficiency somewhat
lower. Early in 1884 there appeared in _Van Nostrand's Engineering
Magazine_ a most valuable paper, by Messrs. Brooks and Steward, with a
preface by Professor Thurston,[3] in which the efficiency was estimated
 at 17 to 18 per cent. of the total heat of combustion. Both these
papers show what I had no opportunity of ascertaining, that is, what
becomes of the 82 per cent. of heat which is not utilized--information
of the greatest importance, as it indicates in what direction
improvement may be sought for, and how loss may be avoided. But, short
as is the time that has elapsed since the appearance of these papers,
you will find that progress has been made, and that a still higher
efficiency is now claimed.

   [Footnote 2: See _Journal_, vol. xxxv, pp. 91, 133.]

   [Footnote 3: Ibid., vol. xliii., pp. 703, 744.]

When I first wrote on this subject, I relied upon some data which led
me to suppose that the heating power of ordinary coal gas was higher
than it really is. At our last meeting, Mr. Hartley proved, by
experiments with his calorimeter, that gas of 16 or 17 candles gave
only about 630 units of heat per cubic foot. Now, if all this heat
could be converted into power, it would yield 630 x 772, or 486,360
f.p.; and it would require only 1,980,000 / 486,360 = 4.07 cubic feet to
produce 1 indicated horse power. Some recent tests have shown that,
with gas of similar heating power, 18 cubic feet have given 1
indicated horse power, and therefore 4.07 / 18 = 22.6 of the whole heat
has been converted--a truly wonderful proportion when compared with
steam-engines of a similar power, showing only an efficiency of 2 to 4
per cent.

The first gas-engine which came into practical use was Lenoir's,
invented about 1866, in which the mixture of gas and air drawn in for
part of the stroke at atmospheric pressure was inflamed by the spark
from an induction coil. This required a couple of cells of a strong
Bunsen battery, was apt to miss fire, and used about 90 cubic feet of
gas per horse power. This was succeeded by Hugon's engine, in which
the ignition was caused by a small gas flame, and the consumption was
reduced to 80 cubic feet. In 1864 Otto's atmospheric engine was
invented, in which a heavily-loaded piston was forced upward by an
explosion of gas and air drawn in at atmospheric pressure. In its
upward stroke the piston was free to move; but in its downward stroke
it was connected with a ratchet, and the partial vacuum formed after
the explosion beneath the piston, together with its own weight in
falling, operated through a rack, and caused rotation of the flywheel.
This engine (which, in an improved form, uses only about 20 cubic feet
of gas) is still largely employed, some 1,600 having been constructed.
The great objection to it was the noise it produced, and the wear and
tear of the ratchet and rack arrangements. In 1876 the Otto-Crossley
silent engine was introduced. As you are aware, it is a single-acting
engine, in which the gas and air are drawn in by the first outward,
and compressed by the first inward stroke. The compressed mixture is
then ignited; and, being expanded by heat, drives the piston outward
by the second outward stroke. Near the end of this stroke the
exhaust-valve is opened, the products of combustion partly escape, and
are partly driven out by the second inward stroke. I say partly, for a
considerable clearance space, equal to 38 per cent. of the whole
cylinder volume, remains unexhausted at the inner end of the cylinder.
When working to full power, only one stroke out of every four is
effective; but this engine works with only 18 to 22 cubic feet of gas
per horse power. Up to the present time I am informed that about
18,000 of these engines have been manufactured. Several other
compression engines have been introduced, of which the best known is
Mr. Dugald Clerk's, using about 20 feet of Glasgow cannel gas. It
gives one effective stroke for every revolution; the mixture being
compressed in a separate air-pump. But this arrangement leads to
additional friction; and the power measured by the brake is a smaller
percentage of the indicated horse power than in the Otto-Crossley
engine. A number of gas engines--such as Bisschop's (much used for
very small powers), Robson's (at present undergoing transformation in
the able hands of Messrs. Tangye), Korting's, and others--are in use;
but, so far as I can learn, all require a larger quantity of gas than
those previously referred to.

[Illustration: OTTO ATMOSPHERIC GAS ENGINE.]

[Illustration: CLERCK'S GAS ENGINE, 6 HORSE POWER.]

[Illustration: OTTO-CROSSLEY GAS ENGINE, 16 H.P.

               Consumption 17.6 cubic feet of 16-candle gas per
               theoretical horse power per hour.

               Average pressure, 90.4 x constant, .568 theoretical
               horse power per pound = 50.8 theoretical horse power.]

[Illustration: ATKINSON'S DIFFERENTIAL GAS ENGINE, 8 H.P.]

I have all along spoken of efficiency as a percentage of the total
quantity of heat evolved by the fuel; and this is, in the eyes of a
manufacturer, the essential question. Other things being equal, that
engine is the most economical which requires the smallest quantity of
coal or of gas. But men of science often employ the term efficiency in
another sense, which I will explain. If I wind a clock, I have spent a
certain amount of energy lifting the weight. This is called "energy of
position;" and it is returned by the fall of the weight to its
original level. In the same way if I heat air or water, I communicate
to it energy of heat, which remains potential as long as the
temperature does not fall, but which can be spent again by a decrease
of temperature. In every heat-engine, therefore, there must be a fall
from a higher to a lower temperature; otherwise no work would be done.
If the water in the condenser of a steam-engine were as hot as that in
the boiler, there would be equal pressure on both sides of the piston,
and consequently the engine would remain at rest. Now, the greater the
fall, the greater the power developed; for a smaller proportion of the
heat remains as heat. If we call the higher temperature T and the
lower T' on the absolute scale, T - T' is the difference; and the
ratio of this to the higher temperature is called the "efficiency."
This is the foundation of the formula we meet so often: E = (T - T')/T.
A perfect heat-engine would, therefore, be one in which the
temperature of the absolute zero would be attained, for (T - O)/T = 1.
This low temperature, however, has never been reached, and in all
practical cases we are confined within much narrower limits. Taking
the case of the condensing engine, the limits were 312 deg. to 102 deg., or
773 deg. and 563 deg. absolute, respectively. The equation then becomes
(773 - 563)/773 = 210/773 or (say) 27 per cent. With non-condensing
engines, the temperatures may be taken as 312 deg. and 212 deg., or 773 deg. and
673 deg. absolute respectively. The equation then becomes (773 - 673)/773
= 100/773, or nearly 13 per cent. The practical efficiencies are not
nearly this, but they are in about the same ratio--27/13. If, then, we
multiply the theoretical efficiencies by 0.37, we get the practical
efficiencies, say 10 per cent. and 5 per cent.; and it is in the
former sense that M. Witz calculated the efficiency of the
steam-engine at 35 per cent.--a statement which, I own, puzzled me a
little when I first met it. These efficiencies do not take any account
of loss of heat before the boiler. In the case of the gas-engine, the
question is much more complicated on account of the large clearance
space and the early opening of the exhaust. The highest temperature
has been calculated by the American observers at 3,443 deg. absolute, and
the observed temperature of the exhaust gases was 1,229 deg.. The fraction
then becomes (3443 - 1229)/3443 = 64 per cent. If we multiply this by
0.37, as we did in the case of the steam-engine, we get 23.7 per
cent., or approximately the same as that arrived at by direct
experience. Indeed, if the consumption is, as sometimes stated, less
than 18 feet, the two percentages would be exactly the same. I do not
put this forward as scientifically true; but the coincidence is at
least striking.

I have spoken of the illuminating power of the gas as of importance;
for the richer gases have also more calorific power, and an engine
would, of course, require a smaller quantity of them. The heat-giving
power does not, however, vary as the illuminating power, but at a much
slower rate; and, adopting the same contrivance as that on which the
absolute scale of temperature is formed, I would suggest a formula of
the following type: H = C (I + K), in which H represents the number of
heat-units given out by the combustion of 1 cubic foot of gas, I is
the illuminating power in candles, and C and K two constants to be
determined by experiment. If we take the value for motive power of the
different qualities of gas as given in Mr. Charles Hunt's interesting
paper in our Transactions for 1882, C might without any great error be
taken as 22 and K as 7.5. With Pintsch's oil gas, however, as compared
with coal gas, this formula does not hold; and C should be taken much
lower, and K much higher than the figures given above. That is to say,
the heating power increases in a slower progression. The data
available, however, are few; but I trust that Mr. Hartley will on
this, as he has done on so many other scientific subjects, come to our
aid.

I will now refer to the valuable experiments of Messrs. Brooks and
Steward, which were most carefully made. Everything was measured--the
gas by a 60 light, and the air by a 300 light meter; the indicated
horse power, by a steam-engine indicator; the useful work, by a Prony
brake; the temperature of the water, by a standard thermometer; and
that of the escaping gases, by a pyrometer. The gas itself was
analyzed; and its heating power calculated, from its composition, as
617.5[theta]. Its specific gravity was .464; and the volume of air was
about seven times that of the gas used (or one-eighth of the mixture),
and was only 111/2 per cent. by weight more than was needed for perfect
combustion. The results arrived at were as follows:

                                          Per cent.
  Converted into indicated horse power,
      including friction, etc.              17.0
  Escaped with the exhaust gas.             15.5
  Escaped in radiation.                     15.5
  Communicated to water in the jacket.      52.0


It will thus be seen that more than half of the heat is communicated
to the water in the jacket. Now, this is the opposite of the
steam-engine, where the jacket is used to transmit heat _to_ the
cylinder, and not _from_ it. This cooling is rendered necessary,
because without it the oil would be carbonized, and lubrication of the
cylinder rendered impossible. Indeed, a similar difficulty has
occurred with all hot-air engines, and is, I think, the reason they
have not been more generally adopted. I felt this so strongly that,
for some time after the introduction of the gas-engine, I was very
cautious in recommending those who consulted me to adopt it. I was
afraid that the wear and tear would be excessive. I have, however, for
some time past been thoroughly satisfied that this fear was needless;
as I am satisfied that a well-made gas-engine is as durable as a
steam-engine, and the parts subject to wear can be replaced at
moderate cost. We have no boiler, no feed pump, no stuffing-boxes to
attend to--no water-gauges, pressure-gauges, safety-valve, or
throttle-valve to be looked after; the governor is of a very simple
construction; and the slide-valves may be removed and replaced in a
few minutes. An occasional cleaning out of the cylinder at
considerable intervals is all the supervision that the engine
requires.

The very large percentage of heat absorbed by the water-jacket should
point out to the ingenuity of inventors the first problem to be
attacked, viz., how to save this heat without wasting the lubricant or
making it inoperative; and in the solution of this problem, I look for
the most important improvement to be expected in the engine. The most
obvious contrivance would be some sort of intercepting shield, which
would save the walls of the cylinder and the rings of the piston from
the heat of the ignited gases. I have just learned that something of
the kind is under trial. Another solution may possibly be found in the
employment of a fluid piston; but here we are placed in a dilemma
between the liquids that are decomposed and the metals that are
oxidized at high temperatures. Next, the loss by radiation--15 per
cent.--seems large; but this is to be attributed to the fact that the
inside surface of the cylinder is at each inward stroke exposed to the
atmosphere--an influence which contributes to the cooling necessary
for lubrication. The remaining 15 per cent., which is carried away by
the exhaust, is small compared with the proportion passing away with
the exhaust steam of a high-pressure or the water of a condensing
engine. As the water in the jacket can be safely raised to 212 deg. Fahr.,
the whole of the jacket heat can be utilized where hot water is
required for other purposes; and this, with the exhaust gases, has
been used for drying and heating purposes.

With such advantages, it may be asked: Why does not the gas-engine
everywhere supersede the steam-engine? My answer is a simple one: The
gas we manufacture is a dear fuel compared with coal. Ordinary coal
gas measures 30 cubic feet to the pound; and 1,000 cubic feet,
therefore, weigh 33 lb. Taking the price at 2s. 9d. per 1,000 cubic
feet, it costs 1d. per lb. The 30 cubic feet at 630[theta] give
19,000[theta] all available heat. Although good coal may yield 14,000
units by its combustion, only about 11,000 of these reach the boiler;
so that the ratio of the useful heat is 11/19. The thermal efficiency
of the best non-condensing engine to that of the gas-engine is in the
ratio 4/22. Multiplying together these two ratios, we get

        11     4        44
        -- x ------- = ----
        19   22_{1/2}  4.28

That is, speaking roughly, 1 lb. of gas gives about ten times as much
power as 1 lb. of coal does in a good non-condensing engine. But at
18s. 8d. a ton we get 10 lb. of coal for 1d.; so that with these
figures the cheapness of the coal would just compensate for the
efficiency of the gas. As to the waste heat passing away from the
engine being utilized, here the gas-engine has no advantage; and, so
far as this is concerned, the gas is about eight times dearer than
coal. The prices of gas and coal vary so much in different places that
it is hard to determine in what cases gas or coal will be the dearer
fuel, considering this point alone.

But there are other kinds of non-illuminating gases--such as Wilson's,
Strong's, and Dowson's--which are now coming into use; and at Messrs.
Crossley's works you will have an opportunity of seeing a large
engineering factory employing several hundred mechanics, and without a
chimney, in which every shaft and tool is driven by gas-engines
supplied by Dowson's gas, and in which the consumption of coal is only
1.2 lb. per indicated horse power. The greatest economy ever claimed
for the steam-engine was a consumption of 1.6 lb.; and this with steam
of very high pressure, expanded in three cylinders successively. Thus
in a quarter of a century the gas-engine has beaten in the race the
steam-engine; although from Watt's first idea of improvement, nearly a
century and a quarter have elapsed.

As regards the steam-engine, it is the opinion of competent
authorities that the limits of temperature between which it works are
so restricted, and so much of the heat is expended in producing a
change of state from liquid to vapor, that little further improvement
can be made. With respect to gas-engines, the limits of temperature
are much further apart. A change of state is not required, and so very
great improvement may still be looked for. It is not impossible even
that some of the younger members of our body may live to see that
period foretold by one of the greatest of our civil engineers--that
happy time when boiler explosions will only be matters of history;
that period, not a millennium removed by a thousand years, but an era
deferred perhaps by only half a dozen decades, when the use of the
gas-engine will be universal, and "a steam-engine can be found only in
a cabinet of antiquities."


_Discussion._

The President said this was a very delightful paper; and nothing could
be finer than Mr. Lane's description of the conversion of heat into
power, and the gradual growth of theory into practical work.

Mr. W. Foulis (Glasgow) agreed that it was admirable; but it required
to be read to be thoroughly appreciated. When members were able to
read it, they would find Mr. Lane had given a very clear description
of the elementary principles of thermo-dynamics in their relation to
the gas-engine and the steam-engine. There was very little in the
paper to raise discussion; but Mr. Lane had made exceedingly clear how
the present loss in a gas-engine was occasioned, and had also shown
how, in the future development of the engine, the loss might be saved,
and the engine rendered more efficient.

Mr. H.P. Holt (of Messrs. Crossley Bros., Limited) said he could
indorse everything Mr. Lane had said. He had found the paper most
interesting and instructive even to himself, though he had some little
practical experience of gas-engines, and was supposed to know a little
about them. He did not pretend to be able to teach other people; but
if he could say anything as to indicator cards, or answer any
questions, he should be happy to do so. (He then described the
indicator diagram of the atmospheric gas-engine.) In this engine the
proportion of the charging stroke to the whole sweep of the piston was
about 10 per cent.; and as the charge drawn in consisted of about 10
per cent. of gas, about 1-100 of the total sweep of the piston was
composed of the gas.

Mr. Foulis asked what proportion the power indicated on the diagram
bore to the power indicated on the brake in the atmospheric engine.

Mr. Holt said unfortunately he had not any figures with him which
would give this information; and it was so long since he had anything
practically to do with this form of engine, that he should not like to
speak from memory. He might add that the largest size of gas-engine
made (of about 100 horse power indicated) was at work at Messrs. Edwin
Butterworth and Co.'s, of Manchester. It was now driven by ordinary
coal gas; but Dowson plant was to be put up very shortly in order to
reduce the cost of working, which, though not excessive, would be
still more economical with the Dowson gas--probably only about 30s.
per week. The present cost was about L4 per week, though it was not
working always at full power.

Mr. T. Holgate (Batley) said he thought it was generally understood,
by those who had studied the subject, that the adoption of compression
of the gaseous mixture before ignition had, so far, more than anything
else, contributed to the improved working of gas-engines. This fact
had not been sufficiently brought out in the paper, although Mr. Lane
had clearly indicated some of the directions in which further
improvements were likely to obtain. Gas engineers were largely
indebted to Mr. Dugald Clerk for the statement he had made of the
theory of the gas-engine.[4] Mr. Lane had given some figures, arrived
at by Messrs. Brooks and Steward, from experiments made in America;
but, prior to these Mr. Clerk had given others which were in the main
in accordance with them. Professor Kennedy had also made experiments,
the results of which agreed with them.[5] The extent of the loss by
the cooling water was thus well ascertained; and it was no doubt by a
reduction of this loss that further improvement in the working of
gas-engines would eventually be obtained.

   [Footnote 4: See Journal, vol. xxxix., p. 648.]

   [Footnote 5: Ibid., vol. xl., p. 955.]

Mr. J. Paterson (Warrington) expressed his appreciation of the paper,
as one of exceptional interest and value. He said he did not rise with
a view to make any observations thereon. The analysis of first
principles required more matured consideration and thought than could
be given to it here. The opinion, however, he had formed of the paper
placed it beyond the reach of criticism. It was now many years since
his attention had been drawn to the name of Denny Lane; and everything
that had come from his facile pen conveyed sound scientific
conclusions. The paper to which they had just listened was no
exception. It was invested with great interest, and would be regarded
as a valuable contribution to the Transactions of the Institute.

Mr. Lane, in reply, thanked the members for the kind expressions used
with respect to his paper. His object in writing it was that any one
who had not paid any attention to the subject before should be able to
understand thoroughly the principles on which gas and hot-air engines
operated; and he believed any one who read it with moderate care would
perfectly understand all the essential conditions of the gas-engine.
He might mention that not long after the thermo-dynamic theory was so
far developed as to determine the amount of heat converted into power,
a very eminent French Engineer--M. Hirn--conducted some experiments on
steam-engines at a large factory, and thought he could account for the
whole heat of combustion in the condensed water and the heat which
passed away; so much so that he actually doubted altogether the theory
of thermo-dynamics. However, being open to conviction, he made further
experiments, and discovered that he had been in error, and ultimately
became one of the most energetic supporters of the theory. This showed
how necessary it was to be careful before arriving at a conclusion on
such a subject. He had endeavored, as far as the nature of the case
allowed, to avoid any scientific abstractions, because he knew that
when practical men came to theory--_x's_ and _y's_, differentials,
integrals, and other mathematical formulae--they were apt to be
terrified.

The President said it was like coming down to every day life to say
that it was important that gas managers should be familiar with the
appliances used in the consumption of gas, and should be able, when
called upon, to give an intelligent description of their method of
working. A study of Mr. Lane's paper would reveal many matters of
interest with regard to this wonderful motor, which was coming daily
more and more into use, not only to the advantage of gas
manufacturers, but of those who employed them.

       *       *       *       *       *




M. MEIZEL'S RECIPROCATING EXHAUSTER.


At the recent Congress of the Societe Technique de l'Industrie du Gaz
en France, M. Meizel, Chief Engineer of the St. Etienne Gas Works,
described a new exhauster devised by him on the reciprocating
principle, and for which he claims certain advantages over the
appliances now in general use. Exhausters constructed on the
above-named principle have hitherto, M. Meizel says, been costly to
fit up, owing to the necessity for providing machinery and special
mechanism for the transmission of motion. This has prevented the
employment of cylinders of large dimensions; and, consequently, when
the quantity of gas to be dealt with has been considerable, the number
of exhausters has had to be increased. The result of this has been
inconvenience, which has led to a preference being shown for other
kinds of exhausters, notwithstanding the manifest advantages which, in
M. Meizel's opinion, those of the reciprocating type possess. The
improvement which he has effected in these appliances consists in the
application to them of cylinders working automatically; and the
general features of the arrangement are shown in the accompanying
illustrations.

[Illustration: IMPROVED RECIPROCATING GAS EXHAUSTER.]

The principal advantages to be gained by the use of this exhauster are
stated by M. Meizel to be the following: Considerably less motive
force is necessary than is the case with other exhausters, which
require steam engines and all the auxiliary mechanism for the
transmission of power. By its quiet and regular action, it prevents
oscillation and unsteadiness in the flow of gas in the hydraulic main,
as well as in the pipes leading therefrom--a defect which has been
found to exist with other exhausters. The bells, being of large area,
serve the purpose of a condenser; and as, owing to its density, the
tar falls to the bottom of the lower vessels, which are filled with
water, contact between the gas and tar is avoided. Although the
appliance is of substantial construction, its action is so sensitive
that it readily adapts itself to the requirements of production. It
may be placed in the open air; and therefore its establishment is
attended with less outlay than is the case with other exhausters,
which have to be placed under cover, and provided with driving
machinery and, of course, a supply of steam.

The total superficial area of the exhauster above described, including
the governor, is 150 square feet; and its capacity per 24 hours is
230,000 cubic feet. It works silently, with an almost entire absence
of friction; and consequently there are few parts which require
lubrication. Exhausters of this type (which, M. Meizel says, could be
made available for ventilation purposes, in case of necessity) may be
constructed of all sizes, from 500 cubic feet per hour upward.

       *       *       *       *       *




AUTOMATIC SIPHON FOR IRRIGATION.


When, at an elevated point in a meadow, there exists a spring or vein
of water that cannot be utilized at a distance, either because the
supply is not sufficient, or because of the permeability of the soil,
it becomes very advantageous to accumulate the water in a reservoir,
which may be emptied from time to time through an aperture large
enough to allow the water to flow in abundance over all parts of the
field.

[Illustration: GIRAL'S AUTOMATIC SIPHON.]

The storing up of the water permits of irrigating a much greater area
of land, and has the advantage of allowing the watering to be effected
intermittingly, this being better than if it were done continuously.
But this mode of irrigating requires assiduous attention. It is
necessary, in fact, when the reservoir is full, to go and raise the
plug, wait till the water has flowed out, and then put in the plug
again as accurately as possible--a thing that it is not always easy to
do. The work is a continuous piece of drudgery, and takes just as much
the longer to do in proportion as the reservoir is more distant from
one's dwelling. In order to do away with this inconvenience, Mr.
Giral, of Langogne (Lozere), has invented a sort of movable siphon
that primes itself automatically, however small be the spring that
feeds the reservoir in which it is placed. The apparatus (see figure)
consists of an elbowed pipe, C A B D E, of galvanized iron, whose
extremity, C, communicates with the outlet, R, where it is fixed by
means of a piece of rubber of peculiar form that allows the other
extremity, B D E, to revolve around the axis, K, while at the same
time keeping the outlet pipe hermetically closed. This rubber, whose
lower extremity is bent back like the bell of a trumpet, forms a
washer against which there is applied a galvanized iron ring that is
fixed to the mouth of the outlet pipe by means of six small screws.
This ring is provided with two studs which engage with two flexible
thimbles, K and L, that are affixed to the siphon by four rivets.
These studs and thimbles, as well as the screws, are likewise
galvanized. Between the branches, A B D E, of the pipe there is
soldered a sheet of galvanized iron, which forms isolatedly a
receptacle or air-chamber, F, that contains at its upper part a small
aperture, _b_, that remains always open, and, at its lower part, a
copper screw-plug, _d_, and a galvanized hook, H.

In the interior of this chamber there is arranged a small leaden
siphon, _a b c_, whose longer leg, _a_, passes through the bottom,
where it is soldered, and whose shorter one, _c_, ends in close
proximity to the bottom. Finally, a galvanized iron chain, G H, fixed
at G to the bottom of the reservoir, and provided with a weight, P, of
galvanized iron, is hooked at H to the siphon and allows it to rise
more or less, according as it is given a greater or less length.

From what precedes, it will be seen that the outlet is entirely
closed, so that, in order that the water may escape, it must pass into
the pipe in the direction, E D B A C.

This granted, let us see how the apparatus works: In measure as the
water rises in the reservoir, the siphon gradually loses weight, and
its extremity, B D H, is finally lifted by the thrust, so that the
entire affair revolves upon the studs, K, until the chain becomes
taut. The apparatus then ceases to rise; but the water, ever
continuing to rise, finally reaches the apex, _b_, of the smaller
siphon, and, through it, enters the air chamber and fills it. The
equilibrium being thus broken, the siphon descends to the bottom,
becomes primed, and empties the reservoir. When the level of the
water, in descending, is at the height of the small siphon, _a b c_,
this latter, which is also primed, empties the chamber, F, in turn, so
that, at the moment the large siphon loses its priming, the entire
apparatus is in the same state that it was at first.

In short, when the water enters the reservoir, the siphon, movable
upon its base, rises to the height at which it is desired that the
flow shall take place. Being arrested at this point by the chain, it
becomes primed, and sinks, and the water escapes. When the water is
exhausted, the siphon rises anew in order to again sink; and this goes
on as long as the period of irrigation lasts.

This apparatus, which is simple in its operation, and not very costly,
is being employed with success for irrigating several meadows in the
upper basin of the Allier.--_Le Genie Civil._

       *       *       *       *       *




ASSAY OF EARTHENWARE GLAZE.


Lead oxide melted or incompletely vitrified is still in common use in
the manufacture of inferior earthenware, and sometimes leads to
serious results. To detect lead in a glaze, M. Herbelin moistens a
slip of white linen or cotton, free from starch, with nitric acid at
10 per cent. and rubs it for ten to fifteen seconds on the side of the
utensil under examination, and then deposits a drop of a solution of
potassium iodide, at 5 per cent. on the part which has been in
contact. A lead glaze simply fused gives a very highly colored yellow
spot of potassium iodide; a lead glaze incompletely vitrified gives
spots the more decided, the less perfect the vitrification; and a
glaze of good quality gives no sensible color at all.--_M. Herbelin._

       *       *       *       *       *




ON THE ELECTRICAL FURNACE AND THE REDUCTION OF THE OXIDES OF BORON,
SILICON, ALUMINUM, AND OTHER METALS BY CARBON.[1]

   [Footnote 1: Read at the recent meeting of the American
   Association, Ann Arbor, Mich.]

By EUGENE H. COWLES, ALFRED H. COWLES, AND CHARLES F. MABERY.


The application of electricity to metallurgical processes has hitherto
been confined to the reduction of metals from solutions, and few
attempts have been made to effect dry reductions by means of an
electric current. Sir W. Siemens attempted to utilize the intense heat
of an electric arc for this purpose, but accomplished little beyond
fusing several pounds of steel. A short time since, Eugene H. Cowles
and Alfred H. Cowles of Cleveland conceived the idea of obtaining a
continuous high temperature on an extended scale by introducing into
the path of an electric current some material that would afford the
requisite resistance, thereby producing a corresponding increase in
the temperature. After numerous experiments that need not be described
in detail, coarsely pulverized carbon was selected as the best means
for maintaining a variable resistance and at the same time as the most
available substance for the reduction of oxides. When this material,
mixed with the oxide to be reduced, was made a part of the electric
circuit in a fire clay retort, and submitted to the action of a
current from a powerful dynamo machine, not only was the oxide
reduced, but the temperature increased to such an extent that the
whole interior of the retort fused completely. In other experiments
lumps of lime, sand, and corundum were fused, with indications of a
reduction of the corresponding metal; on cooling, the lime formed
large, well-defined crystals, the corundum beautiful red, green, and
blue hexagonal crystals.

Following up these results with the assistance of Charles F. Mabery,
professor of chemistry in the Case School of Applied Science, who
became interested at this stage of the experiments, it was soon found
that the intense heat thus produced could be utilized for the
reduction of oxides in large quantities, and experiments were next
tried on a large scale with a current from two dynamos driven by an
equivalent of fifty horse power. For the protection of the walls of
the furnace, which were made of fire brick, a mixture of the ore and
coarsely pulverized gas carbon was made a central core, and it was
surrounded on the sides and bottom by fine charcoal, the current
following the lesser resistance of the central core from carbon
electrodes which were inserted at the ends of the furnace in contact
with the core. In order to protect the machines from the variable
resistance within the furnace, a resistance box consisting of a coil
of German silver wire placed in a large tank of water was introduced
into the main circuit, and a Brush ammeter was also attached by means
of a shunt circuit, to indicate the quantity of current that was being
absorbed in the furnace. The latter was charged by first filling it
with charcoal, making a trough in the center, and filling this central
space with the ore mixture, which was covered with a layer of coarse
charcoal. The furnace was closed at the top with fire brick slabs
containing two or three holes for the escape of the gaseous products
of the reduction, and the entire furnace made air-tight by luting with
fire clay. Within a few minutes after starting the dynamo, a stream of
carbonic oxide issued through the openings, burning usually with a
flame eighteen inches in height. The time required for complete
reduction was ordinarily about an hour.

The furnace at present in use is charged in substantially the same
manner, and the current is supplied by a Brush machine of variable
electromotive force driven by an equivalent of forty horse power. A
Brush machine capable of utilizing 125 horse power, or two and
one-half times as large as any hitherto constructed by the Brush
Electric Company, is being made for the Cowles Electric Smelting and
Aluminum Company, and this machine will soon be in operation.
Experiments already made so that aluminum, silicon, boron, manganese,
magnesium, sodium and potassium can be reduced from their oxides with
ease. In fact, there is no oxide that can withstand temperatures
attainable in this electrical furnace. Charcoal is changed to
graphite. Does this indicate fusion or solution of carbon? As to what
can be accomplished by converting enormous electrical energy into heat
within a limited space, it can only be said that it opens the way into
an extensive field for both pure and applied chemistry. It is not
difficult to conceive of temperatures limited only by the capability
of carbon to resist fusion. The results to be obtained with the large
Brush machine above mentioned will be of some importance in this
direction.

Since the cost of the motive power is the chief expense in
accomplishing reductions by this method, its commercial success is
closely connected with the cheapest form of power to be obtained.
Realizing the importance of this point, the Cowles Electric Smelting
and Aluminum Company has purchased an extensive and reliable water
power, and works are soon to be erected for the utilization of 1,200
horse power. An important feature in the use of these furnaces, from a
commercial standpoint, is the slight technical skill required in their
manipulation. The four furnaces in operation in the experimental
laboratory at Cleveland are in charge of two young men twenty years of
age, who, six months ago, knew absolutely nothing of electricity. The
products at present manufactured are the various grades of aluminum
bronze made from a rich furnace product that is obtained by adding
copper to the charge of ore, silicon bronze prepared in the same
manner, and aluminum silver, an alloy of aluminum with several other
metals. A boron bronze may be prepared by the reduction of boracic
acid in contact with copper.

As commercial results may be mentioned the production in the
experimental laboratory, which averages fifty pounds of 10 per cent.
aluminum bronze daily, and it can be supplied to the trade in large
quantities at prices based on $5 per pound for the aluminum contained,
the lowest market quotation of this metal being at present $15 per
pound. Silicon bronze can be furnished at prices far below those of
the French manufacturers.

The alloys which the metals obtained by the methods above described
form with copper have been made the subject of careful study. An alloy
containing 10 per cent. of aluminum and 90 per cent. of copper forms
the so-called aluminum bronze with a fine golden color, which it
retains for a long time. The tensile strength of this alloy is usually
given as 100,000 pounds to the square inch; but castings of our ten
per cent. bronze have stood a strain of 109,000 pounds. It is a very
hard, tough alloy, with a capacity to withstand wear far in excess of
any other alloy in use. All grades of aluminum bronze make fine
castings, taking very exact impressions, and there is no loss in
remelting, as in the case of alloys containing zinc. The 5 per cent.
aluminum alloy is a close approximation in color to 18 carat gold, and
does not tarnish readily. Its tensile strength in the form of castings
is equivalent to a strain of 68,000 pounds to the square inch. An
alloy containing 2 or 3 per cent. aluminum is stronger than brass,
possesses greater permanency of color, and would make an excellent
substitute for that metal. When the percentage of aluminum reaches 13,
an exceedingly hard, brittle alloy of a reddish color is obtained, and
higher percentages increase the brittleness, and the color becomes
grayish-black. Above 25 per cent. the strength again increases.

The effect of silicon in small proportions upon copper is to greatly
increase its tensile strength. When more than 5 per cent. is present,
the product is exceedingly brittle and grayish-black in color. It is
probable that silicon acts to a certain extent as a fluxing material
upon the oxides present in the copper, thereby making the metal more
homogeneous. On account of its superior strength and high conductivity
for electrical currents, silicon bronze is the best material known for
telegraph and telephone wire.

The element boron seems to have almost as marked an effect upon copper
as carbon does upon iron. A small percentage in copper increases its
strength to 50,000 or 60,000 pounds per square inch without
diminishing to any large extent its conductivity.

Aluminum increases very considerably the strength of all metals with
which it is alloyed. An alloy of copper and nickel containing a small
percentage of aluminum, called Hercules metal, withstood a strain of
105,000 pounds, and broke without elongation. Another grade of this
metal broke under a strain of 111,000 pounds, with an elongation
equivalent to 33 per cent. It must be remembered that these tests were
all made upon castings of the alloys. The strength of common brass is
doubled by the addition of 2 or 3 per cent. of aluminum. Alloys of
aluminum and iron are obtained without difficulty; one product was
analyzed, containing 40 per cent. of aluminum. In the furnace iron
does not seem to be absorbed readily by the reduced aluminum when
copper is present; but in one experiment a mixture composed of old
files, 60 per cent.; nickel, 5 per cent.; and of 10 per cent. aluminum
bronze 35 per cent., was melted together, and it gave a malleable
product that stood a strain of 69,000 pounds.

When the reduction of aluminic oxide by carbon is conducted without
the addition of copper, a brittle product is obtained that behaves in
many respects like pig iron as it comes from the blast furnace. The
same product is formed in considerable quantities, even when copper is
present, and frequently the copper alloy is found embedded in it.
Graphite is always found associated with it, even when charcoal is the
reducing material, and analysis invariably shows a very high
percentage of metallic aluminum. This extremely interesting substance
is at present under examination.

       *       *       *       *       *




THE COWLES ELECTRIC SMELTING PROCESS.


The use of electricity in the reduction of metals from their ores is
extending so rapidly, and the methods of its generation and
application have been so greatly improved within a few years, that the
possibility of its becoming the chief agent in the metallurgy of the
future may now be admitted, even in cases where the present cost of
treatment is too high to be commercially advantageous.

The refining of copper and the separation of copper, gold, and silver
by electrolysis have thus far attracted the greatest amount of
attention, but a commercial success has also been achieved in the dry
reduction by electricity of some of the more valuable metals by the
Cowles Electric Smelting and Aluminum Company, of Cleveland, Ohio.
Both this method of manufacture and the qualities of the products are
so interesting and important that it is with pleasure we call
attention to them as steps toward that large and cheap production of
aluminum that the abundance of its ores and the importance of its
physical properties have for several years made the unattained goal of
many skillful metallurgists.

The Messrs. Cowles have succeeded in greatly reducing the market value
of aluminum and its alloys, and thereby vastly extending its uses, and
they are now by far the largest producers in the world of these
important products. As described in their patents, the Cowles process
consists essentially in the use for metallurgical purposes of a body
of granular material of high resistance or low conductivity interposed
within the circuit in such a manner as to form a continuous and
unbroken part of the same, which granular body, by reason of its
resistance, is made incandescent, and generates all the heat required.
The ore or light material to be reduced--as, for example, the hydrated
oxide of aluminum, alum, chloride of sodium, oxide of calcium, or
sulphate of strontium--is usually mixed with the body of granular
resistance material, and is thus brought directly in contact with the
heat at the points of generation, at the same time the heat is
distributed through the mass of granular material, being generated by
the resistance of all the granules, and is not localized at one point
or along a single line. The material best adapted for this purpose is
electric light carbon, as it possesses the necessary amount of
electrical resistance, and is capable of enduring any known degree of
heat when protected from oxygen without disintegrating or fusing; but
crystalline silicon or other equivalent of carbon can be employed for
the same purpose. This is pulverized or granulated, the degree of
granulation depending upon the size of the furnace. Coarse granulated
carbon works better than finely pulverized carbon, and gives more even
results. The electrical energy is more evenly distributed, and the
current can not so readily form a path of highest temperature, and
consequently of least resistance through the mass along which the
entire current or the bulk of the current can pass. The operation must
necessarily be conducted within an air-tight chamber or in a
non-oxidizing atmosphere, as otherwise the carbon will be consumed and
act as fuel. The carbon acts as a deoxidizing agent for the ore or
metalliferous material treated, and to this extent it is consumed, but
otherwise than from this cause, it remains unimpaired.

Fig. I. of the accompanying drawings is a vertical longitudinal
section through a retort designed for the reduction of zinc ore,
according to this process, and Fig. II. is a front elevation of the
same. Fig. III. is a perspective view of a furnace adapted to
withstand a very high temperature, and Figs. IV. and V. are
respectively longitudinal and transverse sections of the same.

[Illustration: THE COWLES ELECTRIC SMELTING PROCESS.]

This retort consists of a cylinder, A, made of silica or other
non-conducting material, suitably embedded in a body, B, of powdered
charcoal, mineral wool, or of some other material which is not a good
conductor of heat. The rear end of the retort-cylinder is closed by
means of a carbon plate, C, which plate forms the positive electrode,
and with this plate the positive wire of the electric circuit is
connected. The outer end of the retort is closed by means of an
inverted graphite crucible, D, to which the negative wire of the
electric circuit is attached. The graphite crucible serves as a plug
for closing the end of the retort. It also forms a condensing chamber
for the zinc fumes, and it also constitutes the negative electrode.
The term "electrode" is used in this case as designating the terminals
of the circuit proper, or that portion of it which acts simply as an
electrical conductor, and not with the intention of indicating the
ends of a line between which there is no circuit connection. The
circuit between the "electrodes," so called, is continuous, being
established by means of and through the body of broken carbon
contained in the retort, A. There is no deposit made on either plate
of the decomposed constituents of the material reduced. The mouth of
the crucible is closed with a luting of clay, or otherwise, and the
opening, _d_, made in the upper side of the crucible, near its
extremity, comes entirely within the retort, and forms a passage for
the zinc fumes from the retort chamber into the condensing chamber.
The pipe, E, serves as a vent for the condensing chamber. The zinc ore
is mixed with pulverized or granular carbon, and the retort charged
nearly full through the front end with the mixture, the plug, D, being
removed for this purpose.

A small space is left at the top, as shown. After the plug has been
inserted and the joint properly luted, the electric circuit is closed
and the current allowed to pass through the retort, traversing its
entire length through the body of mixed ore and carbon. The carbon
constituents of the mass become incandescent, generating a very high
degree of heat, and being in direct contact with the ore, the latter
is rapidly and effectually reduced and distilled. The heat evolved
reduces the ore and distills the zinc, and the zinc fumes are
condensed in the condensing chamber, precisely as in the present
method of zinc making, with this important exception that, aside from
the reaction produced by heating carbon in the presence of zinc oxide,
the electric current, in passing through the zinc oxide, has a
decomposing and disintegrating action upon it, not unlike the effect
produced by an electric current in a solution. This action accelerates
the reduction, and promotes economy in the process.

Another form of furnace is illustrated by Fig. III., which is a
perspective view of a furnace adapted for the reduction of ores and
salts of non-volatile metals and similar chemical compounds. Figs. IV.
and V. are longitudinal and transverse sections, respectively, through
the same, illustrating the manner of packing and charging the furnace.

The walls and floors L L', of the furnace are made of fire bricks, and
do not necessarily have to be very thick or strong, the heat to which
they are subjected not being excessive. The carbon plates are smaller
than the cross section of the box, as shown, and the spaces between
them and the end walls are packed with fine charcoal.

The furnace is covered with a removable slab of fireclay, N, which is
provided with one or more vents, _n_, for the escaping gases.

The space between the carbon plates constitutes the working part of
the furnace. This is lined on the bottom and sides with a packing of
fine charcoal, O, or such other material as is both a poor conductor
of heat and electricity--as, for example, in some cases, silica or
pulverized corundum or well-burned lime--and the charge, P, of ore and
broken, granular, or pulverized carbon occupies the center of the box,
extending between the carbon plates. A layer of granular charcoal, O',
also covers the charge on top. The protection afforded by the charcoal
jacket, as regards the heat, is so complete, that with the
covering-slab removed, the hand can be held within a few inches of the
exposed charcoal jacket; but with the top covering of charcoal also
removed and the core exposed, the hand cannot be held within several
feet. The charcoal packing behind the carbon plates is required to
confine the heat and to protect them from combustion.

With this furnace, aluminum can be reduced directly from its ores; and
chemical compounds from corundum, cryolite, clay, etc., and silicon,
boron, calcium, manganese, magnesium, and other metals are in like
manner obtained from their ores and compounds. The reduction of ores
according to this process can be practiced, if circumstances require
it, without any built furnace.

At present, the Cowles company is engaged mostly in the producing of
aluminum bronze and aluminum silver and silicon bronze. The plant,
were it run to its full capacity, is capable of turning out eighty
pounds of aluminum bronze, containing 10 per cent. of aluminum daily;
or, were it to run upon silicon bronze, could turn out one hundred and
twenty pounds of that per day, or, we believe, more aluminum bronze
daily than can be produced by all other plants in the world combined.
This production, however, is but that of the experimental laboratory,
and arrangements are making to turn out a ton of bronze daily, and the
works have an ultimate capacity of from eight to ten thousand horse
power. The energy consumed by the reduction of the ore is almost
entirely electrical, only enough carbon being used to unite with the
oxygen of the ore to carry it out of the furnace in the form of the
carbon monoxide, the aluminum remaining behind. Consequently, the
plant necessary to produce aluminum on a large scale involves a large
number of the most powerful dynamos. These are to be driven by
water-power or natural gas and marine engines of great capacity.

The retail price of standard 10 per cent. aluminum bronze is $1 per
pound avoirdupois, which means less than $9 per pound for aluminum,
the lowest price at which it has ever been sold, yet the Cowles
company has laid a proposition before the Government to furnish this
same bronze in large quantities at very much lower prices than this.
The Hercules alloy, castings of which will stand over 100,000 pounds
to the square inch tensile strain, sells at 75 c. a pound, and is also
offered the Government or other large consumers at a heavy discount.
The alloys are guaranteed to contain exactly what is advertised; they
are standardized into 10 per cent., 7.5 per cent., 5 per cent. and 2.5
per cent. aluminum bronze before shipment.

The current available at the Cowles company's works was, until
recently, 330 amperes, driven by an electromotive force of 110 volts
and supplied by two Edison dynamos; but the company has now added a
large Brush machine that has a current of 560 amperes and 52 volts
electromotive force. We shall, on another occasion, give some
particulars of experiments in the reduction of refractory ores by the
process.--_Eng. and Mining Jour._

       *       *       *       *       *




OPTICAL TELEGRAPHY.[1]

   [Footnote 1: Continued from page 8094.]


CRYPTOGRAPHY.--PRESERVATION OF TELEGRAMS.

Optical telegraphy, by reason of its very principle, presents both the
advantage and inconvenience of leaving no automatic trace of the
correspondence that it transmits. The advantage is very evident in
cases in which an optical station falls into the hands of the enemy;
on the other hand, the inconvenience is shown in cases where a badly
transmitted or badly collated telegram allows an ambiguity to stand
subject to dispute. Moreover, in case of warfare between civilized
nations that have all the resources of science at their disposal,
there may be reason to fear lest one of the enemy's optical stations
substitute itself for the corresponding station, and take advantage of
the situation to throw confusion into the orders transmitted. The
remedy for this appears to reside in the use of cryptography and in
the exchange, at various intervals, of certain words that have been
agreed upon beforehand, and that the enemy is ignorant of.

As for the automatic preservation of telegrams, the problem has not
been satisfactorily solved. It has been proposed to connect the key of
the manipulator of the optical apparatus with the manipulator of an
ordinary Morse apparatus, thus permitting the telegram to be preserved
upon a band of paper. It is unnecessary to say that the space occupied
by a dispatch thus transmitted would be considerable; but this is not
what has stopped innovators. The principal objection resides in the
increase in muscular work imposed by this arrangement upon the
telegrapher. Obliged to keep his eye fixed intently at the receiving
telescope, while at the same time maneuvering the manipulator and
spelling aloud the words that he is receiving, the operator should
have a very sensitive manipulator at his disposal, and not be
submitted to mental or physical overtaxation. So the apparatus that
have been devised have not met with much success.

Two French officers, working independently, have hit upon the same
idea of receiving the indications transmitted by the vibration of the
luminous fascicle directly upon their travel. The method consists in
the use of that peculiar property of selenium of becoming a good
conductor under the action of a luminous ray, while in darkness it
totally prevents the passage of the electric current. Such
modification of the physical properties of selenium, moreover, occurs
without the perceptible development of any mechanical work. If, then,
in the line of travel of the luminous fascicle emitted by the optical
apparatus, or in a portion of such fascicle, we interpose a fragment
of selenium connected with the two poles of a local pile, it is easy
to see that the current from the latter will be opened or closed
according as the luminous ray from the apparatus will or will not
strike the selenium, and that the length of time during which the
current passes will depend upon the length of the luminous attacks. A
Morse apparatus interposed in this annexed circuit will therefore give
an automatic inscription of the correspondence exchanged. Such is the
principle. But, practically, very great difficulties present
themselves, these being connected with the rapid weakening of the
electric properties of the selenium, and with the necessity of having
recourse to infinitely small mechanical actions only. The problem is
nevertheless before us, and it is to be hoped that the perseverance of
the scientists who are at work upon it will some day succeed in
solving it.

Finally, we may call attention to the attempts made to receive the
luminous impression upon a band prepared with gelatino-bromide of
silver. In practice this band would unwind uniformly at the focus of
the receiving telescope, which would be placed in a box, forming a
camera obscura. The velocity of this band prepared for photographing
the signals would be regulated by clockwork. The experiments that have
been made have not given results that are absolutely satisfactory, by
reason of the length of the signals received and the mechanical
complication of the device.


OPTICAL TELEGRAPHY BY MEANS OF PROJECTORS.

[Illustration: FIG. 23.]

The projectors employed for lighting to a distance the surroundings of
a stronghold or of a ship have likewise been applied in optical
telegraphy. For this purpose Messrs. Sautter, Lemonnier & Co. have
added to their usual projecting apparatus some peculiar arrangements
that permit of occultations of the luminous focus at proper intervals.
Figs. 21 and 22 show the arrangement of the apparatus, the principle
of which is as follows: When the axis of the projector points toward
the clouds, and in the direction occupied by a corresponding station,
the occultations of the luminous source placed in the focus of the
apparatus produce upon the clouds, which act as a screen, an alternate
series of flashes and extinctions. It is therefore possible with this
arrangement, and by the use of the Morse alphabet, to establish an
optical communication at a distance. The use of this projector (the
principal inconvenience of which is that it requires a clouded sky)
even permits two observers who are hidden from each other by the
nature of the ground to easily communicate at a distance of 36 or 48
miles.


USE OF THE PROJECTOR IN OPTICAL TELEGRAPHY.

[Illustration: FIGS. 21 AND 22.--FRONT VIEW AND LONGITUDINAL SECTION
OF THE MANGIN PROJECTOR.

(Scale 1/15). A. Elliptical mirror. B. Arm of the same. C. Nut for
fixing the mirror. D. Support of the mirror. E. Occultator. F. Support
for same. G. Lever for maneuvering the occultator. I. Support of the
occultator rod. J. Screw for fixing the mirror support. K. Screw for
fixing the support of the occultator rod. L. Screw for fixing the
occultator support.]

The apparatus shown in Figs. 21 and 22 permits of signaling in three
ways:

1. _Upon the Clouds._--In this case the mirror, A, is removed, and the
projector inclined above the horizon in such a way as to illuminate
the clouds to as great a distance as possible. A maneuver of the
occultator, E, between the lamp and the mirror arrests the luminous
rays of the source, or allows them to pass, and thus produces upon the
clouds the dots and dashes of the conventional alphabet.

2. _Isolated Communication by Luminous Fascicles._--When it is desired
to correspond to a short distance of 2 or 3 miles, and establish a
communication between two isolated posts, the mirror, A, is put in
place upon its support, B. The luminous fascicle emanating from the
source reflected by the mirror is thrown vertically. By revolving the
mirror 90 deg. around its horizontal axis the fascicle becomes horizontal,
and may thus be thrown in a given direction at unequal intervals and
during irregular times, and furnish conventional signs.

3. _Night Communication upon the Entire Horizon._--When we wish to
correspond at a short distance, say two miles, and make signals
visible from the entire horizon, the mirror, A, is put in place, so
that it shall reflect the luminous fascicle vertically. The fascicle,
at a distance of about fifty feet, meets a white balloon which it
renders visible from every point in the horizon. The maneuver of the
occultator brings the balloon out of darkness or plunges it thereinto
again, and thus produces the signs necessary for aerial communication.

[Illustration: FIG. 24.]

These ingenious arrangements, which depend upon the state of the
atmosphere, do not appear to have been imitated outside of the navy.


CAPT. GAUMET'S OPTICAL TELEGRAPH.

The system of optical communication proposed by Capt. Gaumet, and
which he names the _Telelogue_, is based upon the visibility of
colored or luminous objects, and upon the possibility of piercing the
opaque curtain formed by the atmosphere between the observer's eye and
a signal, by utilizing the difference in brightness that exists
between such objects and the atmosphere. It is a question, then, of
giving such difference in intensity its maximum of brightness. To do
this, Capt. Gaumet proposes to employ silvered signals upon a black
background. He uses the simple letters of the alphabet, but changes
their value. His apparatus has the form of a large album glued at the
back to a sloping desk. Each silvered letter, glued to a piece of
black cloth, is seen in relief upon the open register. A sort of index
along the side, as in commercial blank-books, permits of quickly
finding any letter at will. Such is the manipulator of the apparatus.

The receiver consists of a spy-glass affixed to the board that carries
the register. For a range of two and a half miles, the complete
apparatus, with a 12x16 inch manipulator and telescope, weighs but
four and a half pounds. For double this range, with a 20x28 inch
manipulator and telescope, the total weight is thirteen pounds. The
larger apparatus, according to the inventor, have a range of seven
miles.

For night work the manipulator is lighted either by one lamp, or by
two lamps with reflector, placed laterally against it.

This apparatus, although well known, and having been publicly
experimented with, has not, to our knowledge, been applied
practically. From a military standpoint, its short range will
evidently not permit it to compete with optical telegraphic apparatus,
properly so called. Perhaps it might rather be of service for private
communications between localities not very far apart, since it costs
but little and is easily operated.


OPTICAL SIGNALING BETWEEN BODIES OF TROOPS.

Optical communications by signals, during day and night, with
experienced men, may, in the absence of telephones, telegraphs, and
messengers, render important service when the distance involved is
greater than two thousand feet.

This mode of correspondence is based upon the use of the Morse
alphabet. The signals are divided into night and day ones. The day
signals are made with small flags. When these are wanting, sheets of
white cardboard may be used. The night signals are made with a lantern
provided with a support, which may be fixed to a wall or upon a
bayonet.

In day signaling, the dashes of the Morse alphabet are formed by means
of two flags (Fig. 23) held simultaneously at arm's length by the
signaler. The dots are formed with a single flag held in the right
hand (Fig. 24). In this way it is possible, by extremely simple
combinations, to establish a correspondence, and produce any
conventional signal. By means of relay stations, the signals may be
transmitted from one to another to a great distance.

In signaling with the lantern, long and short interruptions of the
luminous source are produced by means of a screen.


OPTICAL TELEGRAPHY BY LUMINOUS BALLOONS.

Various interesting experiments have been made with a view to
utilizing luminous captive balloons for optical communications. As we
have already seen, this maybe effected by using opaque balloons, and
throwing upon them at unequal intervals a luminous fascicle by means
of a projector. As for using a luminous source placed in the car of a
balloon, that cannot be thought of in the present state of aeronautic
science; the continual rotation of the balloon around its axis would
render the projection and reception of the signals in a given
direction impossible.


OPTICAL TELEGRAPHY IN THE MARINE.

For communicating optically from ship to ship during the day, the
marine uses flags of different forms and colors, and flames. Between
ships and the land there are used what are called semaphore signals,
which are made by means of a mast provided with three arms and a disk
placed at the upper part. The combinations of signs thus obtained,
which are analogous in principle to those of the Chappe telegraph,
permit of satisfactorily communicating to a distance.

On board ship, hand signals are used like those employed by the army
for communicating between bodies of troops. For night communications
the marine employs lights corresponding to the day flags, as well as
rockets, and luminous rays projected by means of reflectors and
intercepted by screens.

In conclusion, it may be said that optical telegraphy, which has only
within a few years emerged from the domain of theory to enter that of
practice, has taken a remarkable stride in the military art and in
science. It is due to its processes that Col. Perrier has in recent
years been enabled to carry out certain geodesic work that would have
formerly been regarded as impracticable, notably the prolongation of
the arc of the meridian between France and Spain. Very recently, an
optical communication established between Mauritius and Reunion
islands, to a distance of 129 miles, with 24 inch apparatus, proved
that, in certain cases, the costly laying of a submarine cable may be
replaced by the direct emission of a luminous ray.

       *       *       *       *       *




A NEW STYLE OF SUBMARINE TELEGRAPH.


Mr. F. Von Faund-Szyll has devised an original system of submarine
telegraph, which is based upon the well known property that selenium
exhibits of modifying its resistance under the influence of luminous
rays, and which he styles the _Selen-Differenzialrecorder_.

Contrary to what is found in the other systems hitherto employed, the
Faund-Szyll system utilizes the cable current merely for starting the
receiving apparatus, which are operated by means of strong local
batteries. The result is that the mechanical work that devolves upon
the line current, which is, as well known, very weak, is exceedingly
reduced.

The system consists of two essential parts: (1) The receiver, properly
so called. (2) The relay as well as the registering apparatus or
_differenzialrecorder_. The receiver consists of a closed box, K, in
the interior of which there is a very intense source of light whose
rays escape by passing through apertures, _a a'_, in the front part
(Fig. 1).

As a source of light, there may be conveniently employed an
incandescent lamp, _g_, capable of giving an intense light, and
arranged (as shown in Fig. 2) behind the side that contains the slits,
_a a'_.

The starting apparatus consists of a small galvanometric helix, _r_,
analogous to Thomson's siphon recorder, which is suspended from a
cocoon fiber and capable of moving in an extremely powerful magnetic
field, N S. This helix carries, as may be seen in Figs. 1, 3 and 4, a
prolongation, _v_, at its lower end whose form is that of a prism, and
which is arranged in front of the partition of the box, K, in such a
way that it exactly covers the two slits, a and _a_ when the bobbin is
at rest, and in this case prevents the luminous rays of the lamp, _g_,
from escaping from the box. But, as soon as the current sent through
the cable reaches the spirals of the bobbin, through the conductors,
_y y'_, the sum of the elementary electrodynamic actions that arise
causes the helix to revolve to the right or left, according to the
polarity of the current, while at the same time the helix slightly
approaches one or the other of the poles of the magnet. The
prolongation, _v_, of the helix, being firmly united with the latter,
follows it in its motion, and has the effect of permitting the
luminous rays to escape through one or the other of the slits, _a a'_,
so that the freeing of the luminous fascicle, if such an expression is
allowable, is effected.

[Illustration: FIG. 1.]

In order to prevent oscillations, which could not fail to occur after
each emission of a current (so that the helix, instead of returning to
a position of equilibrium and stopping there, would go beyond it and
alternately uncover the slits, _a a'_), the apparatus is provided with
a liquid deadener. To this end, the prolongation, _v_, carries a
piece, _o_, which dips into a cup containing a mixture of glycerine
and water.

We shall now describe the _differenzialrecorder_. Opposite the two
slits, _a_ and _a'_, there are two powerful converging lenses, _l_ and
_l'_, whose foci coincide with two sorts of selenium plate rheostat,
_z_ and _z'_. The result of this arrangement is that as soon as one of
the slits, as a consequence of the displacement of the helix, _r_,
allows a luminous fascicle to escape, this latter falls upon the
corresponding lens, which concentrates it and sends it to the selenium
plates just mentioned. Under the influence of the luminous rays, the
resistance that the selenium offers to the passage of an electric
current instantly changes. At M and M' are placed two horseshoe
magnets whose poles are provided with pieces of soft iron that serve
as cores to exceedingly fine wire bobbins, _d_. These polarized pieces
are arranged in the shape of a St. Andrew's cross, and in such a way
that the poles of the same name occupy the two extremities of the same
arm of the cross, an arrangement very clearly shown in Fig. 2.

[Illustration: FIG. 2.]

Between the poles of the magnets, M and M', there is a permanent
magnet, A, movable around a vertical axis, _i_. Four spiral springs,
_f_, whose tension may be regulated, permit of centering this latter
piece in such a way that when the current is traversing the spirals of
the polar bobbins it is equally distant from the four poles, _n_, _s_,
_s'_, and _n'_. Under such circumstances it is evident that a
difference in the power of attraction of these four poles, however
feeble it be, will result in moving the magnet, A, in one direction or
the other around its axis. The energy and extent of such motion may,
moreover, be magnified by properly acting upon the four regulating
springs.

The bobbins of the magnet, M, are mounted in series with the selenium
plates, _z_, the local battery, B, and a resistance box, W. Those of
the magnet, M', are in series with _z'_, B', and W'. The local
batteries, B and B', are composed of quite a large number of elements.
The current from the battery, B, traverses the selenium plates and the
bobbins of the magnet, M, and returns to B through the rheostat, W;
and the same occurs with the current from B'. The two currents, then,
are absolutely independent of one another.

From this description it is very easy to see how the system works. Let
us suppose, in fact, that the current which is traversing the spirals
of the helix, _r_, has a direction such that the helix in its movement
approaches the pole, S; then the prolongation, _v_, will uncover the
slit, _a_, which, along with _a'_, had up to this moment been closed,
and a luminous fascicle escaping through _a_ will strike the lens,
_l'_, and from thence converge upon the selenium plates, _z'_. This is
all the duty that the line current has to perform.

The luminous rays, in falling upon the selenium plates, _z'_, modify
the resistance that these offered to the passage of the current
produced by the battery, B'. As this resistance diminishes, the
intensity of the current in the circuit supplied by the battery, B',
increases, the attractive action of the polar pieces of the magnet,
M', diminishes, the equilibrium is destroyed, and the piece, A,
revolves around the axis, _i_. If the polarity of the line current
were different, the same succession of phenomena would occur, save
that the direction of A's rotation would be contrary. As for the
rheostats, W W', their object is to correct variations in the
selenium's resistance and to balance the resistances of the two
corresponding circuits. The magnet, A, will be combined with a
registering apparatus so as to directly or indirectly actuate the
printing lever. The entire first part of this apparatus, which is very
sensitive, may be easily protected from all external influence by
placing it in a box, and, if need be, in a room distant from the one
in which the employes work.

[Illustration: FIGS. 3 AND 4.]

The _differenzialrecorder_ alone has to be in the work room.

As may be seen, the system is not wanting in originality. Experience
alone will permit of pronouncing upon the question as to whether it is
as practical as ingenious.--_La Lumiere Electrique._

       *       *       *       *       *




A NEW CIRCUIT CUTTER.


Messrs. Thomson & Bottomley have recently invented a peculiar circuit
cutter based upon the use of a metal whose melting point is
exceedingly low. Recourse is had to this process for breaking the
current within as short a time as possible. In this new device the
ends of the conductors are soldered together with the metal in
question at one or several points of the circuit. The metal employed
is silver or copper of very great conductivity, seeing that the
increase of temperature in a conductor, due to a sudden increase of
the current, is inversely proportional to the product of the electric
resistance by the specific heat of the conductor; that these metals
are best adapted for giving constant and definite results; and that
the contacts are better than with lead or the other metals of low
melting point which are frequently employed in circuit cutters.

[Illustration: FIG. 1.]

Fig. 1 represents one form of the new device. Here, a is the copper or
silver wire, and _b_ is a soldering made with a very fusible metal and
securing a continuity of the circuit. Each extremity of the wire, _a_,
is connected with a heavy ring, _c_, of copper or other good
conducting metal. The hook, _d_, with which the upper ring, _c_, is in
contact, communicates metallically with one of the extremities of the
conductor at the place where the latter is interrupted for the
insertion of the circuit cutter. The hook, _e_, with which the lower
ring, _c_, is in contact, tends constantly to descend under the action
of a spiral spring, _f_, which is connected metallically with the
other extremity of the principal conductor. The hooks, _d_ and _e_,
are arranged approximately in the same vertical plane, and have a
slightly rounded upper and lower surface, designed to prevent the
rings, _c_, of the fusible wire, _a_, from escaping from the hooks. In
Fig. 1 the position of the arm, _e_, when there is no fusible wire in
circuit, is shown by dotted lines. When this arm occupies the position
shown by entire lines, it exerts a certain traction upon the
soldering, _b_, and separates the two halves of the wire, _a_, as soon
as the intensity of circulation exceeds its normal value. The mode of
putting the wire with fusible soldering into circuit is clearly shown
in the engraving.

[Illustration: FIG. 2.]

Fig. 2 shows a different mode of mounting the wire. The wire, _q_, is
soldered in the center, and is bent into the shape of a U, and kept in
place by the pieces, _r_ and _s_. In this way the two ends of it tend
constantly to separate from each other. Messrs. Thomson & Bottomley
likewise employ weights, simply, for submitting the wire to a constant
stress. The apparatus is inclosed in a box provided with a glass
cover.--_La Lumiere Electrique._

       *       *       *       *       *




NEW MICRO-TELEPHONIC APPARATUS.


Despite the simplicity of their parts, and the slight value of the
materials employed, the existing micro-telephonic apparatus keep at
relatively high prices, and the use of them is often rejected, to the
benefit of speaking tubes, when the distance between stations is not
too great. We propose to describe a new style of apparatus that are in
no wise inferior to those in general use, and the price of which is
relatively low.

The microphone transmitter may have several forms. The most elementary
of these consists of two pieces of carbon, from one to one and a
quarter inches in length by one-half inch in width, between which are
fixed two _nails_, about two inches in length, whose extremities,
filed to a point, enter small conical apertures in the carbons. Fig. 1
gives an idea of the arrangement.

[Illustration: FIG. 1.]

Fig. 2 represents a model which is a little more complicated, but
which gives remarkable results. The largest nail is here two inches in
length, and the shortest three-quarter inch.

[Illustration: FIG. 2.]

The receivers may be Bell telephones of the simplest form found in the
market (Fig. 3); but for these there may be substituted a bar of soft
iron, cast iron, or steel, one of the extremities of which is provided
with a bobbin upon, which is wound insulated copper wire 0.02 inch in
diameter. The apparatus is mounted like an ordinary Bell telephone. A
horseshoe electro may also be used, and the poles be made to act (Fig.
4). The current sent by the transmitter suffices to produce a magnetic
field in which the variations in intensity produced by the microphone
succeed perfectly in reproducing speech and music. With four Leclanche
elements, the sounds are perceived very clearly. The elements used may
be bichromate of potash ones, those of Lelande and Chaperon, etc.

[Illustration: FIG. 3.--RECEIVER.]

[Illustration: FIG. 4.]

To this apparatus there may be added a second bobbin of coarser wire
into which is passed a current from a local pile. This produces a much
intenser magnetic field, and, consequently, louder sounds. This
modification, however, is really useful only for long distances.

Any arrangement imaginable may be given the transmitter and receiver;
but, aside from the fact that the ones just indicated are the
simplest, they give results that are at least equal, if not superior,
to all others.

We shall insist here only upon the arrangement of the microphone,
which is new (at least in practice), and upon the uselessness of
having well magnetized steel bars and wires of extreme fineness in the
receiver.

[Illustration: FIG. 5.]

We have stated that the nail microphones are the simplest. The nails
may be replaced by copper or any other metal, or they may be well
nickelized; but common nails answer very well, and do not oxidize
much. An apparatus of this kind (Fig. 5) that has been for more than a
year in a laboratory filled with acid vapors is yet working very well.
These apparatus possess the further advantage of being very strong,
and of undergoing violent shocks without breaking or even getting out
of order. They may be used either with or without induction coils. We
have not yet measured their range, but can cite the following fact:

One of these apparatus, quite crudely mounted, was put into a circuit
with a resistance of 300 ohms. With a single already exhausted
bichromate element, giving scarcely 2 volts, musical sounds and speech
reached the receiver without being notably weakened. Such resistance
represents a length of eighteen miles of ordinary telegraph wire.
After this, 700 ohms were overcome with 3.4 volts. This result was
obtained by direct transmission, and without an induction coil, and it
is probable that it might be much exceeded without sensibly increasing
the electromotive force of the current.--_Le Genie Civil._

       *       *       *       *       *




MESSRS. KAPP AND CROMPTON'S MEASURING INSTRUMENTS.


We give herewith, from the _Elektrotechnische Zeitschrift_, a few
interesting details in regard to the measuring apparatus of Messrs.
Kapp and Crompton.

It is evident that when we use permanent magnets or springs as
directing forces in measuring instruments, we cannot count upon an
absolute constancy in the indications, as the magnetism of the
magnetized pieces, or the tension of the springs, modifies in time.
The apparatus require to be regulated from time to time, and hence the
idea of substituting electro-magnets for permanent ones.

[Illustration: FIG. 1.]

If we suppose (Fig. 1) a magnetized needle, _n s_, placed between the
extremities of a soft iron core, N S, and if we group the circuit in
such a way that the current, after traversing the coil, _e e_, of the
electro, traverses a circle, _d d_, situated in a plane at right
angles with the plane of the needle's oscillation, it is evident that
we shall have obtained an apparatus that satisfies the aforesaid
conditions. It seems at first sight that in such an instrument the
directing force should be constant from the moment the electro was
saturated, and it would be possible, were sufficiently thin cores
used, to obtain a constancy in the directing magnetic field for
relatively feeble intensities. In reality, the actions are more
complex. The needle, _n s_, is, in fact, induced to return to its
position of equilibrium by two forces, the first of which (the
attraction of the poles, N S) rapidly increases with the intensity so
as to become quickly and perceptibly constant, while the second (the
sum of the elementary electrodynamic actions that are exerted between
the spirals, _e e_, and the needle, _n s_) increases proportionally to
the intensity of the current. If we represent these two sections
graphically by referring the magnetic moments as ordinates and the
current intensities as abscissas to two co-ordinate axes (Fig. 2), we
shall obtain for the first force the curve, O A B, which, starting
from A, becomes sensibly parallel with the axis of X, and for the
second the right line, O D. The resultant action is represented by the
curve, O E E'_F. It will be seen that this action, far from being
constant, increases quite rapidly with the intensity of the current,
so that the deflections would become feebler and feebler for strong
intensities, of current; and this, as well known, would render the
apparatus very defective from a practical point of view.

[Illustration: FIG. 2.]

But the action of the spirals can be annulled without sensibly
diminishing the magnetism of the core by arranging a second system of
spirals identical with the first, but placed in a plane at right
angles therewith, or, more simply still, by having a single system of
spirals comprising the coil of the electro-magnet, but distributed in
a plane that is oblique with respect to the needle's position of rest.
It then becomes possible, by properly modifying such angle of
inclination, to obtain a total directing action that shall continue to
increase with the intensity, and which, graphically represented, shall
give the curve, O G G'_H, for example (Fig. 2).

[Illustration: FIG. 3.]

[Illustration: FIG. 4.]

[Illustration: FIG. 5.]

This arrangement, which is adopted in Mr. Kapp's instruments, gives
very good results, as may be easily seen by reference to Figs. 3 and
4, in which the current intensities or differences of potential are
referred as ordinates and the degrees of deflection of the needle as
abscissas. The unbroken lines represent the curves obtained with the
apparatus just described, while the dotted ones give the curve of
deflection of an ordinary tangent galvanometer. These curves show that
for strong intensities of current Mr. Kapp's instrument is more
advantageous than the tangent galvanometer. Mr. Crompton has
constructed an amperemeter upon the same principle, which is shown in
Fig. 5.--_La Lumiere Electrique._

       *       *       *       *       *




THE CHEMICAL ACTION OF LIGHT.


Professor A. Vogel, in a communication to the "Sitzungsberichte der
Munchener Akademie," brings into prominence the fact that the hemlock
plant, which yields coniine in Bavaria, contains none in Scotland.
Hence he concludes that solar light plays a part in the generation of
the alkaloids in plants. This view is corroborated by the circumstance
that the tropical cinchonas, if cultivated in our feebly lighted
hothouses, yield scarcely any alkaloids. Prof. Vogel has proved this
experimentally. He has examined the barks of cinchona plants obtained
from different conservatories, but has not found in any of them the
characteristic reaction of quinine. Of course it is still possible
that quinine might be discovered in other conservatory-grown
cinchonas, especially as the specimens operated upon were not fully
developed. But as the reaction employed indicates very small
quantities of quinine, it may be safely assumed that the barks
examined contained not a trace of this alkaloid, and it can scarcely
be doubted that the deficiency of sunlight in our hothouses is one of
the causes of the deficiency of quinine.

It will at once strike the reader as desirable that specimens of
cinchonas should be cultivated in hothouses under the influence of the
electric light, in addition to that of the sun.

If sunlight can be regarded as a factor in the formation of alkaloids
in the living plant, it has, on the other hand, a decidedly injurious
action upon the quinine in the bark stripped from the tree. On drying
such bark in full sunlight the quinine is decomposed, and there are
formed dark-colored, amorphous, resin-like masses. In the manufacture
of quinine the bark is consequently dried in darkness.

This peculiar behavior of quinine on exposure to sunlight finds its
parallel in the behavior of chlorophyl with the direct rays of the
sun. It is well known that the origin of chlorophyl in the plant is
entirely connected with light, so that etiolated leaves growing in the
dark form no chlorophyl. But as soon as chlorophyl is removed from the
sphere of vegetable life, a brief exposure to the direct rays of the
sun destroys its green color completely.

Prof. A. Vogel conjectures that the formation of tannin in the living
plant is to some extent influenced by light. This supposition is
supported by the fact that the proportion of tannin in beech or larch
bark increases from below upward--that is, from the less illuminated
to the more illuminated parts, and this in the proportions of 4:6 and
5:10.

Sunny mountain slopes of a medium height yield, according to wide
experience, on an average the pine-barks richest in tannin. In woods
in level districts the proportion of tannin is greatest in localities
exposed to the light, while darkness seems to have an unfavorable
effect. Here, also, we must refer to the observation that leaves
exceptionally exposed to the light are relatively rich in tannin.

We may here add that in the very frequent cases where a leaf is
shadowed by another in very close proximity, or where a portion of a
leaf has been folded over by some insect, the portion thus shaded
retains a pale green color, while adjacent leaves, or other portions
of the same leaf, assume their yellow, red, or brown autumnal tints.
If, as seems highly probable, these tints are due to transformation
products of tannin, we may not unnaturally conclude that they will be
absent where tannin has not been generated.--_Jour. of Science._

       *       *       *       *       *




EUTEXIA.[1]

   [Footnote 1: Read before the Birmingham Philosophical Society,
   January 22, 1885.]

By THOMAS TURNER, Assoc. R.S.M., F.C.S., Demonstrator of Chemistry,
Mason College.


There are a number of interesting facts, some of which are known to
most persons, and many of them have been long recognized, of which,
however, it must be owned that the explanation is somewhat obscure,
and the connections existing between them have been but recently
pointed out. As an example of this, it is well known that salt water
freezes at a lower temperature than fresh water, and hence sea-water
may be quite liquid while rivers and ponds are covered with ice.
Again, it is noticed that mixtures of salts often have a fusing-point
lower than that of either of the constituent salts, and of this fact
we often take advantage in fluxing operations. Further, it is well
known that certain alloys can be prepared, the melting-points of which
are lower than the melting-point of either of the constituent metals
alone. Thus, while potassium melts at 62.5 deg. C., and sodium at about
98 deg., an alloy of these metals is fluid at ordinary temperatures, and
fusible metal melts below the temperature of boiling water, or more
than 110 deg. lower than the melting-point of tin, the most fusible of the
three metals which enter into the composition of this alloy. But
though these and many similar facts have been long known, it is but
recently, owing largely to the labors of Dr. Guthrie, that fresh
truths have been brought to light, and a connection shown to exist
throughout the whole which was previously unseen, though we have still
to acknowledge that at present there is much at the root of the matter
which is but imperfectly understood. Still Dr. Guthrie proves a
relationship to exist between the several facts we have previously
mentioned, and also between a number of other phenomena which at first
sight appear to be equally isolated and unexpected, and we are asked
to regard them all as examples of what he has called "eutexia."

We may define a eutectic substance as a body composed of two or more
constituents, which constituents are in such proportion to one another
as to give to the resultant compound body a minimum temperature of
liquefaction--that is, a lower temperature of liquefaction than that
given by any other proportion.[2] It will be seen at once by this
definition that the temperature of liquefaction of a eutectic
substance is lower than the temperature of liquefaction of either or
any of the constituents of the mixture. And, further, it is plain that
those substances only can be eutectic which we can obtain both as
liquid and solid, and hence the property of eutexia is closely
connected with solution.

   [Footnote 2: Guthrie, _Phil. Mag._ [5], xvii., p. 462.]

Following in the natural divisions adopted by Dr. Guthrie, we may
consider eutexia in three aspects:


I. CRYOHYDRATES.

If a _dilute_ aqueous saline solution be taken at ordinary
temperatures, and then slowly cooled to some point below zero on the
Centigrade scale, the following series of changes will in general be
observed: On reaching a point below zero, the position of which is
dependent upon the nature of the salt and the amount of dilution, it
will be found that ice is formed; this will float upon the surface of
the solution, and may be readily removed. If the ice so removed be
afterward pressed, or carefully drained, it will be found to consist
of nearly pure water, the liquid draining away being a strong saline
solution which had become mechanically entangled among the crystals of
ice during solidification. If we further cool the brine which remains,
we notice a tolerably uniform fall of temperature with accompanying
formation of ice. But at length a point is reached at which the
temperature ceases to fall until the whole of the remaining
mother-liquor has solidified, with the production of a compound called
a cryohydrate,[3] which possesses physical properties different from
those of either the ice or the salt from which it is formed.

   [Footnote 3: Guthrie, _Phil. Mag._, 4th Series, xlix., pp. 1,
   206, 266; 5th Series, i., pp. 49, 354, 446, vi., p. 35.]

If, on the other hand, we commence with a _saturated_ saline solution,
in general it is noticed on cooling the liquid a separation of salt
ensues, which salt sinks to the bottom of the mass, and may be
removed. The salt so separating may be either anhydrous or a "hydrate"
of greater concentration than the mother-liquor. So long as this
separation proceeds the temperature falls, but at length a point is
reached at which the thermometer remains stationary until the whole is
solidified, with the production of a cryohydrate. This temperature of
solidification is the same whether we start with a dilute or a
saturated solution, and the composition of the cryohydrate is found to
be constant. The temperature of production of the cryohydrate is
identical with the lowest temperature which can be produced on
employing a mixture of ice and the salt as a freezing mixture or
cryogen.

It will be readily seen that in the formation of a cryohydrate we have
an example of eutexia, since the constituents are present in such
proportion as to give to the resultant compound body a minimum
temperature of liquefaction.


II. EUTECTIC SALT ALLOYS.[4]

   [Footnote 4: F. Guthrie, _Phil. Mag._ [5], xvii., p. 469; F.B.
   Guthrie, _Journ. Chem. Soc_,. 1885, p. 94.]

Although it has been long known that on mixing certain salts the
resulting substance possessed a lower melting-point than either of the
constituent salts alone, still but few determinations of the
melting-points of mixtures of salts have been made, and even these are
often of small value, on account of the very considerable range of
temperature observed during solidification. This is due largely to the
fact that eutectic mixtures were not known, as equivalent proportions
of various salts have been employed, while eutectic mixtures are
seldom found to possess any simple arithmetical molecular relationship
between their constituents.

Eutectic salt alloys closely resemble cryohydrates in behavior. If for
simplicity we confine our attention to a fused mixture of two salts in
any proportion other than eutectic, it is found that, on cooling, the
thermometer falls steadily, until at length that salt which is in
excess of the proportion required for a eutectic mixture begins to
separate out. If this is removed, the thermometer falls until a fixed
point is reached at which the temperature remains stationary until the
whole of the mixture solidifies. On remelting, the temperature of
solidification is found to be quite fixed, and the mixture is
evidently eutectic.

It is of interest to notice that from our knowledge of the
cryohydrates it becomes possible to predict the existence,
composition, and temperature of solidification of a eutectic alloy, if
we are previously furnished with the melting-points of mixtures of the
substances in question. Or, in other cases, we may predict from the
curve of melting-points that no eutectic alloy is possible.

As an example, we may take the determinations of the melting-points of
mixtures of potassium and sodium nitrate by M. Maumene.[5] These are
graphically represented in Fig. 1, the curve being derived from the
mean of the temperatures given in the memoir. From this diagram we
should be led to expect a eutectic mixture, since the curve dips below
a horizontal line passing through the melting-point of the more
fusible of its constituents. From our curve we should expect a
eutectic mixture with about 35 per cent. KNO_{3}, and with a
temperature of solidification below 233 deg.. Dr. Guthrie gives 32.9 per
cent. at 215 deg.. This agreement is as good as might be expected when one
remembers that the melting-points, not being of eutectic mixtures, are
difficult to determine, and a considerable range is given; that
analyses of mixtures of potassium and sodium salts are apt to vary;
and that the two observers differ by +-7 deg. in the temperatures given for
the melting-points of the original salts.

   [Footnote 5: _Comptes Rendus_, 1883, 2, p. 45.]

[Illustration: FIG. 1.]

Dr. Tilden has drawn my attention to an interesting example of the
lowering of melting-point by the mixture of salts. The melting-point
of monohydrochloride of turpentine oil is 125 deg., while that of the
dihydrochloride is 50 deg.; but on simply stirring together these
compounds in a mortar at common temperatures, they immediately
liquefy. Two molecules of the monohydrochloride and one molecule of
the dihydrochloride form a mixture which melts at about 20 deg..


III. EUTECTIC METALLIC ALLOYS.

Although many fusible alloys have been long known, I believe no true
eutectic metallic alloy had been studied until Dr. Guthrie[6] worked
at the subject, employing the same methods as with his cryohydrates.
It is found if two metals are fused together and the mixture allowed
to cool, that the temperature falls until a point is reached at which
that metal which is present in a proportion greater than is required
to form the eutectic alloy begins to separate. If this solid be
removed as it forms, the temperature gradually falls until a fixed
point is reached, at which the eutectic alloy solidifies. Here the
thermometer remains stationary until the whole has become solid, and,
on remelting, this temperature is found to be quite fixed. In addition
to the di-eutectic alloys, we have also tri- and tetra-eutectic
alloys, and as an example of the latter we may take the
bismuth-tin-lead-cadmium eutectic alloy, melting at 71 deg..

   [Footnote 6: _Phil. Mag._, 5th Series, xvii., p. 462.]

We have already seen with salt eutectics that, given the curve of
melting-points of a mixture in various proportions, we may predict the
existence, composition, and melting-point of the eutectic alloy. As a
matter of course, the same thing holds good for metallic eutectics. An
interesting example of this is furnished by the tin-lead alloys, the
melting-points of which have been determined by Pillichody.[7] From
these determinations we obtain the curve given in Fig. 2, and from
this curve, since it dips below a horizontal line passing through the
melting-point of the more fusible constituent, we are at once able to
predict a eutectic alloy. We should further expect this to have a
constitution between PbSn_{3} and PbSn_{4} and a melting-point
somewhat below 181 deg.. On melting together tin and lead, and allowing
the alloy to cool, we find our expectation justified; for by pouring
off the fluid portion which remains after solidification has
commenced, and repeating this several times with the portion so
removed, we at length obtain an alloy which solidifies at the constant
temperature of 180 deg., when the melting-point of tin is taken as 228 deg..
On analysis 1.064 grm. of this alloy gave 0.885 grm. SnO_{2}, which
corresponds to Sn 65.43 per cent., or PbSn_{3.3}. This, therefore, is
the composition of the eutectic alloy, and it finds its place
naturally on the curve given in Fig. 2.

   [Footnote 7: _Dingler's Polyt. Journ._, 162, p. 217;
   _Jahresberichte_, 1861, p. 279.]

[Illustration: FIG. 2.]

It will be seen that the subject of eutexia embraces many points of
practical importance and of theoretical interest. Thus it has been
shown by Dr. Guthrie that the desilverizing of lead in Pattinson's
process is but a case of eutexia, the separation of lead on cooling a
bath of argentiferous lead poor in silver being analogous to the
separation of ice from a salt solution. Dr. Guthrie has also shown
that eutexia may reasonably be supposed to have played an important
part in the production and separation of many rock-forming minerals.

It is with considerable diffidence that I suggest the following as an
explanation of the multitude of facts to which previous reference has
been made.

In a mixture of two substances, A and B, we have the following forces
active, tending to produce solidification:

    1. The cohesion between the particles of A.

    2. The cohesion between the particles of B.

    3. The cohesion between the particles of A and the particles of B.

With regard to this last factor, it will be seen that there are three
cases possible:

    1. The cohesion of the mixture A B may be greater than the
    cohesion of A + the cohesion of B.

    2. The cohesion of A B may be equal to the cohesion of A + the
    cohesion of B.

    3. The cohesion of A B may be less than the cohesion of A + the
    cohesion of B.

Now, since cohesion tends to produce solidification, we should in the
first case expect to find the melting-point of the mixture _higher_
than the mean of the melting-points of its constituents, or the curve
of melting-points would be of the form given in _a_, Fig. 3. Here no
eutectic mixture is possible.

[Illustration: FIG. 3.]

In the second case, where cohesion A B = cohesion A + B, we should
obtain melting-points for the mixture which would agree with the mean
of the melting-points of the constituents, the curve of melting-points
would be a straight line, and again no eutectic mixture would be
possible.

In the third case, however, where cohesion A B is less than cohesion A
+ B, we should find the melting-points of the mixture lower than the
mean of the melting-points of its constituents, and the curve of
melting-points would be of the form given in _e_, Fig. 3. Here, in
those cases where the difference of cohesion on mixture is
considerable, the curve of melting-points may dip below the line _e
f_. This is the _only case_ in which a eutectic mixture is possible,
and it is, of course, found at the lowest point of the curve.

If it be true, as above suggested, that the force of cohesion is at
its minimum in the eutectic alloy, we should expect to find, in
preparing a eutectic substance, either that actual expansion took
place, or that the molecular volume would gradually increase in
passing along our curve of melting-points, from either end, for each
molecule added, and that it would obtain its greatest value at the
point corresponding to the eutectic alloy.

Of this I have no direct evidence as yet, but it is a point of
considerable interest, and I may possibly return to it at some future
time.--_Chemical News._

       *       *       *       *       *




CHINOLINE.


Dr. Conrad Berens, of the University of Pennsylvania, reaches the
following:

 1. Chinoline tartrate is a powerful agent, producing death by
asphyxia.

 2. The drug increases the force and frequency of the respirations by
stimulating the vagus roots in the lung.

 3. It paralyzes respiration finally by a secondary depressant action
upon the respiratory center.

 4. It does not cause convulsions.

 5. It lessens and finally abolishes reflex action by a direct action
upon the cord, and by a slight action upon the muscles and nerves.

 6. It diminishes or abolishes muscular contractility respectively
when applied through the circulation or directly.

 7. It coagulates myosin and albumen.

 8. It causes insalivation by paralysis of the secretory fibers of the
chorda tympani; increases the flow of bile; has no action upon the
spleen.

 9. It lowers blood-pressure by paralyzing the vaso-motor centers and
by a direct depressant action upon the heart muscle.

 10. It diminishes the pulse rate by direct action upon the heart.

 11. It lowers the temperature by increasing the loss of heat.

 12. It is a powerful antiseptic; and, finally,

 13. Its paths of elimination are not known.

       *       *       *       *       *




METHOD FOR RAPID ESTIMATION OF UREA.


Being called upon to make a good many brief and rapid analyses of
urine on "clinic days" of our medical department, I devised the
following modification of Knop's method of estimating urea; and after
using it for a year with perfectly satisfactory results, venture to
describe and recommend it as especially adapted for physicians' use,
by reason of simplicity, cheapness, and accuracy. In perfecting and
testing it I was assisted greatly by J. Torrey, Jr., then working with
me.

[Illustration]

The apparatus consists of the glass tube, A, which is about 8 cm. long
and 21/2 cm. in diameter, joined to the tube, B, which is about 25 or 30
cm. in length in its longer arm and 8 or 10 in its shorter, and has a
diameter of about 5 mm. Near the bend is an outlet tube, _c_, provided
with "ball valve" or pinch cock. _d_, _e_, _f_, _g_, are marks upon the
tubes. C is a rubber cork with two holes through which the bent tube,
D, passes. D is of such size and length as to hold about 1 c.c., and
one of its ends may be a trifle longer than the other.

The apparatus is used as follows: Remove the cork and pour in mercury
until it stands at _e_ and _g_, then fill up to the mark, _f_, with
sodium or potassium hypobromite (made by shaking up bromine with a
strong solution of sodium or potassium hydroxide). Next carefully fill
the tube in the cork with the urine, being careful especially not to
run it over or leave air bubbles in it. This can easily be done by
using a small pipette, but if accidentally a little runs over, it
should be wiped off the end of the cork with blotting paper. The cork
is then to be inserted closely into the tube; the urine tube being so
small, the urine will not run out in so doing. The mercury is then
drawn out through _c_ till it stands in B at _d_. Its level in A will
of course not be changed greatly. Now, incline the apparatus till the
surface of the hypobromite touches the urine in the longer part of the
urine tube, and then bring it upright again. The urine will thus be
discharged into the hypobromite, which will of course decompose the
urea, liberating nitrogen, which will cause the mercury to rise in B.
Shake until no further change of level is seen, and mark the level of
mercury in B with a rubber band, then remove the cork, draw out the
liquid with a pipette, dry out the tube above the mercury with scrap
of blotting paper, pour back the mercury drawn out, and repeat the
process to be sure that no error was made.

If now two or three marks have been made upon the tube, B, indicating
the height of the mercury when solutions containing known per cents.
of urea are used, an accurate opinion can be at once formed as to the
condition of the urine as regards urea.

As is well known, normal urine contains about 2.5-3 per cent. of urea,
so that graduations representing 2, 2.5, 3, and 4 per cent. are
usually all that are needed, though of course many more can be easily
made.

The results obtained with this apparatus have been repeatedly compared
with those of more elaborate ones, and no practical difference
observed. Evidently the same apparatus, differently graduated, might
be employed to determine the carbonate present in such a substance as
crude soda ash or other similar mixture. In such a case the weighed
material would be put upon the mercury with water and the small tube
filled with acid.

Bowdoin College Chemical Laboratory.--_F.C. Robinson, in Amer. Chem.
Jour._

       *       *       *       *       *

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