CHAPTER II.

SYPHON TUBE BAROMETERS.

=30. Principle of.=--If some mercury, or any other fluid, be poured into a

tube of glass, bent in the form of =U=, and open at both ends, it will

rise to the same height in both limbs, the tube being held vertically. If

mercury be poured in first, and then water upon it at one end, these

liquids will not come to the same level; the water will stand much higher

than the mercury. If the height of the mercury, above the line of meeting

of the fluids, be one inch, that of the water will be about

thirteen-and-a-half inches. The explanation of this is, that the two

columns balance each other. The pressure of the atmosphere in each limb is

precisely similar; but the one column stands so much higher than the

other, because the fluid of which it is composed is so much lighter, bulk

for bulk, than the other. If one end of the tube be hermetically closed,

the other limb be cut off within a few inches of the bend, and the tube

carefully filled with mercury; by placing it in a vertical position, the

mercury will fall, if the closed limb be long enough, until it is about

thirty inches higher than that in the exposed limb, where it will remain.

Here the atmosphere presses upon the short column; but not upon the long

one. It is this pressure, therefore, which maintains the difference of

level. In fact, it forms a barometer without a cistern, the short limb

answering the purpose of a cistern. The first barometers on this principle

were devised by the celebrated philosopher, Dr. Hook, as described in the

next section.

31. DIAL, OR WHEEL BAROMETERS.

The familiar household "Weather Glasses" are barometers on the syphon

principle. The portions of the two limbs through which the mercury will

rise and fall with the varying pressure of the atmosphere are made of

precisely the same diameter; while the part between them is contracted. On

the mercury, in the exposed limb, rests a round float of ivory or glass;

to this a string is attached and passed over and around a brass pulley,

the other end carrying another lighter weight. The weight resting on the

mercury rises and falls with it. On the spindle of the pulley, which

passes through the frame and centre of the dial-plate, is fixed a light

steel hand, which revolves as the pulley turns round. When the mercury

falls for a decrease of atmospheric pressure, it rises by the same

quantity in the short tube, and pushes up the float, the counterpoise

falls, and thus moves the hand or pointer to the left. When the pressure

increases, the pointer is drawn in a similar manner to the right.

[Illustration: Fig. 18.]

[Illustration: Fig. 19.]

[Illustration: Fig. 20.]

The dials are generally made of metal silvered over or enamelled, but

porcelain may be used. If the circumference of the pulley, or "wheel," be

two inches, it will revolve once for an alteration of level amounting to

two inches in each tube, or four inches in the height of the barometric

column; and as the dial may be from twenty to thirty-six inches in

circumference, five to nine inches on the graduated scale corresponds to

one inch of the column; and hence the sub-divisions are distinctly

perceptible, and a vernier is not necessary.

The motion of the pointer alone is visible; and a mahogany, or rosewood,

frame, supports, covers, and renders the instrument ornamental and

portable. In the back of the frame is a hinged door, which covers the

cavity containing the tube and fixtures. The dial is covered by a glass in

a brass rim, similar to a clock face. A brass index, working over the

dial, moveable by a key or button, may be applied, and will serve to

register the position of the hand when last observed. These instruments

are usually fitted with a thermometer, and a spirit level; the latter for

the purpose of getting the instrument perfectly vertical. They sometimes

have, in addition, a hygrometer, a sympiesometer, an aneroid, a mirror, or

a clock, &c., singly or combined. The frame admits of much variety of

style and decoration. It may be carved or inlaid. The usual adjustment of

scale is suited for localities at no considerable elevation above the

sea. Accordingly, being commercial articles, they have been found

frequently quite out of place. When intended for use at high elevations,

they should have a special adjustment of scale. As household instruments

they are serviceable, and ornamental. But the supply-and-demand principle

upon which they are sold, has entailed upon those issued by inferior

makers a generally bad adjustment of scale. The illustrations are those of

ordinary designs.

[Illustration: Fig. 21.]

[Illustration: Fig. 22.]

[Illustration: Fig. 23.]

Dial barometers required for transmission to distant parts, as India and

the Colonies, are furnished with a steel stop-cock, to render them

portable more effectually than can be done by the method of _plugging_ the

tube.

32. STANDARD SYPHON BAROMETER.

Fig. 24 represents the most accurate form of the Gay Lussac barometer. The

short limb is closed at the top, after the mercury is introduced, and a

small lateral puncture is made at _a_, which is covered over with a

substance which permits the access of air, but prevents the escape of any

mercury when the instrument is packed for travelling. The bent part of the

tube is contracted to a capillary bore; and just above this, in the long

limb, is placed the air-trap, already described (see p. 17), and here

illustrated (fig. 25). When reversed, as it must be for portability, the

capillary attraction keeps the mercury in the long branch. Should the

mercury of the short column get detached, some small quantity of air _may_

pass; but it will be arrested at the pipette, and will not vitiate the

length of the barometric column. It can be easily expelled by gently

shaking or tapping the instrument before suspending it for observation. In

the illustration, the zero of the scale is placed at Z, near the middle of

the tube; and the graduations extend above and below. In making an

observation, it is necessary to take the reading ZA on the long branch,

and ZB on the short one. The sum of the two gives the height of the

barometer. The zero of the scale in some instruments is placed low down,

so as to require the difference of the two readings to be taken. A

thermometer is attached to the frame as usual.

[Illustration: Fig. 24.]

[Illustration: Fig. 25.]

These instruments can be very accurately graduated, and are very exact in

their indications, provided great care has been exercised in selecting the

tubes, which must be of the same calibre throughout the parts destined to

measure the variations of atmospheric pressure. They should be suspended

so as to insure their hanging vertically.

The syphon barometer does not require correction for capillarity nor for

capacity, as each surface of the mercury is equally depressed by capillary

attraction, and the quantity of mercury which falls from the long limb of

the tube occupies the same length in the short one. The barometric height

must, however, be corrected for temperature, as in the cistern barometer.

Tables containing the temperature corrections to be applied to barometer

readings for scales engraved on the glass tube, or on brass or wood

frames, are published.

A Treatise on Meteorological Instruments Explanatory of Their Scientific Principles, Method of Construction, and Practical Utility · 第 2 / 16 章