DESCRIPTION OF A MERCURIAL AIRHOLDER.

Suggested by an inspection of Mr. WATT’S Machine for containing

Factitious Airs.

_By WILLIAM CLAYFIELD_.

Several modes of counteracting the pressure of a decreasing column of

mercury having been thought of in conjunction with Mr. W. Cox, the

following was at last adopted as the most simple and effectual.

Plate 1 Fig. 1, represents a section of the machine, which consists of

a strong glass cylinder A cemented to one of the same kind B, fitted

to the solid block C, into which the glass tube D is cemented for

conveying air into the moveable receiver E.

The brass axis F, Fig. 2, having a double bearing at _a_, _a_, is

terminated at one end by the wheel G, the circumference of which is

equal to the depth of the receiver, so that it may be drawn to the

surface of the mercury by the cord _b_ in one revolution; to the other

end is fitted the wheel H, over which the balance cord _c_ runs in an

opposite direction in the spiral groove _e_, a front view of the wheel

H is shewn at Fig. 3.

Having loaded the receiver with the weight I, something heavier than

may be necessary to force it through the mercury, it is balanced by

the small weight K, which hangs from that part of the spiral where the

radius is equal to that of the wheel G, from this point the radius

of the spiral must be increased in such proportion, that in every

part of its circuit, the weight K may be an exact counterpoise to the

airholder. In this way, so little friction will be produced, that

merely plunging the lower orifice of the tube D under mercury contained

in the small vessel L, will be sufficient to overcome every resistance,

and to force the gas discharged from the beak of a retort into the

receiver, where whatever may be its quantity, it will be subjected to

a pressure exactly corresponding to that of the atmosphere. The edge

of the wheel H being graduated, the balance cord _c_ may be made to

indicate its volume.

Should it at any time be necessary to reduce the pressure to the medium

standard of the barometer, it may easily be done by graduating the

lower end of the tube D, and adding to the weights I or K, as may be

found necessary; the surface of the mercury in the tube pointing out

the increase or diminution.

The concavity at the top of the internal cylinder is intended to

contain any liquid it may be thought proper to expose to the action of

the gas.

The upper orifice _f_, with its ground stopper, is particularly useful

in conveying air from the retort _g_, with its curved neck, into the

receiver, without its passing through the tube D. In all cases where a

rapid extrication of gas is expected the retort _g_, should be firmly

luted to the orifice and the weight I, removed from the top of the

receiver, this by diminishing the pressure, will admit the gas to

expand freely in the airholder at the instant of its formation, and

prevent an explosion of the vessels. The same caution must be observed

whenever any inflammation of gas is produced by the electric spark.

The air may be readily transferred through water or even mercury by the

tube _h_, Fig. 1.

To prevent an absorption of mercury in case of a condensation taking

place in the retort made use of for generating air, Mr. Davy has

applied the stop-cock _i_, to which the neck is firmly luted. This

stop-cock is likewise of great service in saturating water with acid or

alkaline gases, which may be effected by luting one end of the tube _k_

to the stop-cock, and plunging the other into the fluid in the small

vessel _l_, cemented at top, and terminating in the bent funnel _m_—the

tube _h_ having been previously removed, and the lower orifice of the

tube D either sunk to a considerable depth in mercury, or closed with a

ground stopper. The bend of the funnel _m_, may be accurately closed by

the introduction of a few lines of mercury.

The application of the stop-cock _n_, has enabled Mr. Davy to perform

some experiments on respiration with considerable accuracy.

_Note._ This apparatus was first described in

the third part of Dr. Beddoes’s Considerations;

its relation to Mr. Davy’s experiments with the

improvements it has lately received, may probably be

deemed sufficient to excuse the re-printing it.—The

weight I. Fig. 2, having been omitted in the plate,

the reader must supply the deficiency.

W. C.

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