The art of glass-blowing : $b or Plain instructions for making the chemical and philosophical instruments which are formed of glassDanger, T.-P.
Science
The art of glass-blowing : $b or Plain instructions for making the chemical and philosophical instruments which are formed of glass
Danger, T.-P.
Glass blowing and working
The hydrometers with two, three, and four branches, are graduated by
having their tubes divided into a hundred or a thousand equal parts.
The divisions on each branch must correspond with those on the other
branches.
* * * * *
GRADUATION OF BAROMETERS.--The graduation of this instrument consists
in dividing a piece of metal, wood, or ivory, into inches and parts of
inches. The divided rod is then employed to measure the height of the
mercury in the tube. As the rule is moveable, the operation presents no
sort of difficulty: all that is necessary is to make the zero of the
scale coincide with the inferior level of the mercury; the point which
corresponds with the superior level of the mercury, seen in the tube,
indicates the height of the barometric column. It is in this manner
that the cistern barometer is graduated.
But if the barometer is one of those in which the surface of the
mercury is variable, such as the barometer of Gay-Lussac, it is
necessary to have recourse to a different process of graduation. If
the two branches of the instrument are very regular, and of equal
diameter, you first measure with precision the height of the column of
mercury, then divide it in the middle, and fix the scale, which must be
graduated in such a manner that the mark of fifteen inches corresponds
exactly with the middle point. This mode of graduation serves to
indicate merely the apparent height of the barometric column. If you
desire that the scale should immediately indicate the real height, you
must fix the zero at the middle of the column, and then double the
figure which marks each degree.
When you do not wish to write the real height, you make two divisions,
of which one proceeds upwards, the other downwards. You do not, in this
case, double the value of each division, but in observations made with
such a barometer scale you add the degree marked by the two surfaces,
in order to find the real height.
It is in an analogous manner that you graduate the gauges or short
barometers which are employed to measure the density of air under
the recipient of the air-pump. You take the height of the mercury in
the gauge, and fix at the middle of the column the zero of a double
scale, of which one division proceeds upwards, the other downwards;
or, instead of this, if you choose to have only one scale, and that an
ascending scale, you double the value of every degree.
The zero of the barometric scale can be fixed below the inferior
surface of the mercury; but then, to have the real height, it is
necessary to measure precisely the height of the mercury in the two
branches of the instrument, and to deduct the smaller from the larger.
Public-domain text, read in full here on John Shaqi.
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