An instrument for ascertaining the specific gravities of different liquids. The most common description of these instruments consists of a hollow ball, of either metal or glass, capable of floating in any known liquid, and having two stems, the lower one terminating in a weight, in order that the instrument may float with the stems upright, and the upper stem (which is of the same diameter throughout), being graduated, to show the density of the fluid by the depth to which it sinks; as the heavier fluids will buoy up the instrument more than such as are lighter. In this way, however, it is clear that the stem must be of considerable thickness, in order that the instrument may have an extensive range, in which case the smaller differences of density will not be perceptible. To obviate this imperfection various contrivances have been resorted to; one of the most common of which is, to construct the instrument as above described, but with a very slender stem, which is divided into 100 equal parts; and to provide a number of movable rings, all of equal weight, any one of which being slipped over the stem, when the instrument floats in distilled water with zero on the stem at the surface of the water, will cause it to descend until the top of the scale be at the surface; and the density is estimated by the number of weights required to bring the lower part of the scale below the surface, minus the number of divisions of the scale which remain above the surface.

But the method of Fahrenheit is both simpler and more accurate. The hydrometer of Fahrenheit consists of a hollow ball with a counterpoise below, and a very slender stem above, terminating in a small dish. The middle or half length (the stem,) is distinguished by a fine line across, and the instrument is always immersed up to this line by placing weights in the little dish above. Then as the part immersed is constantly of the same magnitude, and the whole weight of the hydrometer is known, this last weight added to the weights in the dish will be equal to the weight of fluid displaced; and if the gravity of water be represented by 1000, and the weight be divided into thousandth parts of the weight of the instrument when it sinks to the middle of the stem in distilled water, the number of weights required to sink the instrument to the mark on the stem when floating in any fluid, added to the weight of the instrument, or 1000, will represent the specific gravity of the fluid.

The engraving on the following page represents an instrument for ascertaining specific gravities, invented by Dr. Hare, Professor of Chemistry in the University of Pennsylvania. This instrument, to which the inventor has given the name of Litrameter, owes its efficiency to the principle, that when columns of different liquids are elevated by the same pressure, their heights must be inversely as their gravities. Two glass tubes, of the size and bore usually employed in barometers, are made to communicate internally with each other, and with a gum elastic bag G, by means of a brass tube, and two sockets of the same metal, into which they are severally inserted. The brass tube terminates in a cock, in which the neck of the bag is tied. Between the cock and the glass tubes there is a tube at right angles to an opening into that which connects them. At the lower end of this tube, a small copper rod R enters through a collar of leather. The tubes are placed vertically in grooves, against an upright strip of wood, tenonned into a pedestal of the same material.

Parallel to one of the grooves, in which the tubes are situated, a strip of brass is fastened, and graduated, so that each degree may be equal to 1/220 of the whole height of the tubes.

The brass plate is long enough to admit of about 140°. Close to this scale a vernier v is made to slide, so that the divisions of the scale are susceptible of sub-division into tenths, and the whole height of the tubes into about 2200 parts or degrees. On the left side of the tube there is another strip of brass, with another set of numbers, so situated as to comprise two degrees of the scale above mentioned, in one. Agreeably to this enumeration the height of the tubes is, by the aid of a correspondent graduation on the vernier, divided into 1100 parts or degrees. A small strip of sheet-tin k is let into a kerf in the wood, supporting the tubes, in order to indicate the commencement of the scale; and the depth to which the orifices of the tubes must extend. At distances from this of 1000 parts and 2000 parts, (commensurate with those of the scale,) there are two other indices, T T, to the right hand tube. Let a small vessel containing water be made to receive the lower end of the tube, by the side of which the scale is situated; and a similar vessel of any other fluid, whose gravity is sought, be made to receive the lower end of the other tube; so that the end of the one tube may be covered by the liquid in question, and the end of the other tube by the water.

The bag being compressed, a great part of the contained air is expelled through the tubes, and rises through the liquid in the tumblers. When the bag is allowed to resume its shape, the consequent rarefaction allows the liquids to rise into the tubes, in obedience to the greater pressure of the atmosphere without. If the liquid to be assayed be heavier than water (as, for instance, let it be concentrated sulphuric acid,) it should be raised a little above the first index, at the distance of 1000 degrees from the common level of the orifices of the tubes. The vessels holding the liquids being then removed, so | that the result may be uninfluenced by any inequality in the height of the liquids, the column of acid must be lowered, until its upper surface coincide exactly with the index 1000. Opposite the upper surface of the column of water the two first numbers of specific gravity of the acid will then be found; and, by duly adjusting and inspecting the vernier, the third figure will be ascertained. The liquids should be at the temperature of 60°. If the liquid under examination be lighter than water, as in the case of pure alcohol, it must be raised to the upper index.

The column of water, measured by the scale of 1000, will then be found at 800 nearly; which shows that 1000 parts of alcohol are, in weight, equivalent to 800 parts of water; or, in other words, 800 is ascertained to be the specific gravity of the alcohol. The sliding rod and tube at r, between the cock and the glass tubes, facilitates the adjustment to the index of the column of liquid in the right hand glass tube. When the rod is pushed in as far as possible, it causes a small leak, by which the air enters; and the columns of the liquids, previously raised too high by the bag, may be allowed to fall, till the liquid which is to be assayed is near the index; then, by pushing the rod in, they may be gradually lowered, and adjusted to the proper height, with great accuracy. A rod of this kind, graduated, might answer the purpose of a vernier.

Hydrometer 686

Meikles' Syphon Hydrometer, represented in the annexed engraving, it will be seen, is upon this same principle, but of a much simpler construction. This instrument consists of a glass tube, open at both ends, and bent into a kind of double syphon, having four parallel legs; so that the open ends are pointed in the same direction, or upwards, as in the annexed engraving. The manner of using it is very simple: let one of the ends be stopped with a finger or cock, and water be poured into the other. The fluid will only rise a small way into the second leg, because of the included air: next, stop the other orifice, and open the one first closed; and having poured into the latter the liquid whose specific gravity is to be tried, open the top of the water tube; then the instrument being held upright, the two liquids will arrange themselves so as to press equally on the included air. This pressure will be measured by the difference in the heights of the two columns of either liquids multiplied by its specific gravity, so that by dividing the difference of the two columns of water by the difference of those of the other liquid, we obtain the specific gravity of the latter; that of water being unity.

The difference between the columns may be measured by applying any scale of small equal parts, or the glass may be attached to a graduated plate furnished with verniers, etc. The longer the columns of liquid employed, the more accurate the process. The expansion of the glass or its capillary action cannot affect the result, nor is it influenced by the expansion of the scale; the only correction required will be to reduce the observations to one temperature.