A simple kind of hydrometer is very much used at sea, as “a sea-water test;” and as the observations are usually recorded in a meteorological register or the ship’s log-book, it may not be altogether out of place to give a description of it here.
It is cons
The indications depend upon the hydrostatic principle, that floating bodies displace a quantity of the fluid which sustains them equal to their own weight. According, therefore, as the specific gravities of fluids differ from each other, so will vary the quantities of the fluids displaced by the same body when floated successively in each.
The specific gravity of distilled water, at the temperature of 62° F, being taken as unity, the depth to which the instrument sinks when gently immersed in such water is the zero of the scale. The graduations extend from 0 to 40; the latter being the mark which will be level with the surface when the instrument is placed in water, the specific gravity of which is 1·040. In recording observations, the last two figures only—being the figures on the scale—are written down. Sea-water usually ranges from 1·020 to 1·036.
A small tin, copper, or glass cylinder is useful for containing the water to be tested. It should be wider than the hydrometer, and always filled to the brim. If fitted to a stand, which is supported by gimbals, it will be very convenient. Water in a bucket, basin, or other wide vessel, acquires motion at sea, and the eye cannot be brought low enough (on account of the edges) to read off the scale accurately.
Errors of observation may occur with the hydrometer, if it be put into water without being clean, or without being carefully wiped. The instrument is extremely accurate if correctly used. It should be kept free from contact with the sides of the vessel; and all dust, smears, or greasiness, should be scrupulously avoided, by carefully wiping it with a clean cloth before and after use.
Whenever the temperature of the water tested differs from 62°, a correction to the reading is necessary, for the expansion or contraction of the glass, as well as the water itself, in order to reduce all observations to one generally adopted standard.
Negretti and Zambra’s hydrometer, with thermometer in the stem, shows the density and temperature in one instrument.
For the following Tables we are indebted to the kindness of Admiral FitzRoy:—
Table for reducing observations made with a Brass Hydrometer, assuming the linear expansion of brass to be 0·000009555 for 1° F. The correction is additive for all temperatures above 62°, and subtractive for temperatures below 62°.
t° | Correction. | t° | Correction. | t° | Correction. | t° | Correction. |
32 | -0·0014 | 48 | -0·0010 | 64 | +0·0002 | 80 | +0·0020 |
33 | ·0014 | 49 | ·0009 | 65 | ·0003 | 81 | ·0021 |
34 | ·0014 | 50 | ·0009 | 66 | ·0004 | 82 | ·0023 |
35 | ·0014 | 51 | -0·0008 | 67 | ·0005 | 83 | ·0024 |
36 | ·0014 | 52 | ·0008 | 68 | +0·0006 | 84 | ·0026 |
37 | ·0014 | 53 | ·0007 | 69 | ·0007 | 85 | +0·0027 |
38 | -0·0014 | 54 | ·0006 | 70 | ·0008 | 86 | ·0029 |
39 | ·0013 | 55 | ·0006 | 71 | ·0009 | 87 | ·0030 |
40 | ·0013 | 56 | -0·0005 | 72 | ·0010 | 88 | ·0032 |
41 | ·0013 | 57 | ·0004 | 73 | ·0011 | 89 | ·0033 |
42 | ·0013 | 58 | ·0003 | 74 | +0·0013 | 90 | +0·0035 |
43 | ·0012 | 59 | ·0003 | 75 | ·0014 | 91 | ·0036 |
44 | -0·0012 | 60 | ·0002 | 76 | ·0015 | 92 | ·0038 |
45 | ·0011 | 61 | -0·0001 | 77 | ·0016 | 93 | ·0040 |
46 | ·0011 | 62 | 0·0000 | 78 | ·0018 | 94 | ·0041 |
47 | -0·0010 | 63 | +0·0001 | 79 | +0·0019 | 95 | +0·0043 |
Table for reducing observations made with a Glass Hydrometer, assuming the linear expansion of glass to be 0·00000463 for 1° F. The correction is additive for temperatures above 62°, and subtractive for temperatures below 62°.
t° | Correction. | t° | Correction. | t° | Correction. | t° | Correction. |
32 | -0·0019 | 48 | -0·0012 | 64 | +0·0002 | 80 | +0·0023 |
33 | ·0019 | 49 | ·0011 | 65 | ·0003 | 81 | ·0024 |
34 | ·0018 | 50 | ·0011 | 66 | ·0004 | 82 | ·0026 |
35 | ·0018 | 51 | -0·0010 | 67 | ·0005 | 83 | ·0027 |
36 | ·0018 | 52 | ·0009 | 68 | +0·0007 | 84 | ·0029 |
37 | ·0017 | 53 | ·0008 | 69 | ·0008 | 85 | +0·0031 |
38 | -0·0017 | 54 | ·0008 | 70 | ·0009 | 86 | ·0032 |
39 | ·0017 | 55 | ·0007 | 71 | ·0010 | 87 | ·0034 |
40 | ·0016 | 56 | -0·0006 | 72 | ·0012 | 88 | ·0036 |
41 | ·0016 | 57 | ·0005 | 73 | ·0013 | 89 | ·0037 |
42 | ·0015 | 58 | ·0004 | 74 | +0·0014 | 90 | +0·0039 |
43 | ·0015 | 59 | ·0003 | 75 | ·0016 | 91 | ·0041 |
44 | -0·0014 | 60 | ·0002 | 76 | ·0017 | 92 | ·0042 |
45 | ·0014 | 61 | -0·0001 | 77 | ·0018 | 93 | ·0044 |
46 | ·0013 | 62 | 0·0000 | 78 | ·0020 | 94 | ·0046 |
47 | -0·0013 | 63 | +0·0001 | 79 | +0·0021 | 95 | +0·0048 |
158. NEWMAN’S SELF-REGISTERING TIDE-GAUGE.
At places where the phenomena of the tides are of much maritime importance, a continuous series of observations upon the rise and fall, and times of change, is essentially necessary as a basis for the construction of good tide tables; and as such observations should also be accompanied with the registration of atmospheric phenomena, we have no hesitation in inserting a description of an accurate self-registering tide-gauge.
The tide-gauge, as shown in the illustration, consists of a cylinder, A, which is made to revolve on its axis once in twenty-four hours by the action of the clock, B. A chain, to which is attached the float, D, passes over the wheel, C, and on the axis of this wheel, C (in about the middle of it) is a small toothed wheel, placed so as to be in contact with a larger toothed wheel carrying a cylinder, E, over which passes another smaller chain. This chain, passing along the upper surface of the cylinder, A, and round a second cylinder, F, at its further end, is acted on by a spring so as to be kept in a constant state of tension. In the middle of this chain a small tube is fixed for carrying a pencil, which, being gently pressed down by means of a small weight on the top of it, performs the duty of marking on paper placed round the cylinder the progress of the rise or fall of the tide as the cylinder revolves, and as it is drawn by the chain forward or backward by the rise or fall of the float. The paper is prepared with lines equidistant from each other, to correspond with the hours of the clock, crossed by others showing the number of feet of rise and fall.
The cylinder while in action revolves from left to right to a spectator facing the clock, and the pencil is carried horizontally along the top of the cylinder; and the large wheel being made to revolve by the rise and fall of the float, turns the wheel with the small cylinder, E, attached to it. If the tide is falling, the small chain is wound round the cylinder, E, and the pencil is drawn towards the large wheel; but if the tide is rising, the small chain is wound on to the cylinder, F, by means of the spring contained in it, which constantly keeps it in a state of tension. Thus, by means of the rise and fall of the tide, a lateral progress is given to the pencil, while the cylinder is made to revolve on its axis by the clock, so that a line is traced on the paper showing the exact state of the tide continuously, without further attention than is necessary to change the paper once every day, and to keep the pencil carefully pointed; or a metallic pencil may be used, which will require little, if any, attention.
A good self-registering tide-gauge is a valuable and important acquisition wherever tidal observations are required, and the only perfectly efficient instrument of this kind is that invented by the late Mr. John Newman, of Regent Street, London. It is now in action in several parts of the world, silently and faithfully performing its duty, requiring no other kind of attention than that of a few minutes daily, and thus admitting the employment of the person on any other service whose duty it would otherwise have been to have registered the tide. It has done much by its faithful records in contributing to the construction of good tide tables for many places; for those unavoidable defects dependent on merely watching the surface on a divided scale are set aside by it, all erroneous conclusions excluded, and a true delineation of Nature’s own making is preserved by it for the theorist.
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