Classics of modern science : $b (Copernicus to Pasteur)
History
Classics of modern science : $b (Copernicus to Pasteur)
Science; Science -- History
In Dr. Priestley’s last volume of experiments is related an experiment
of Mr. Warltire’s, in which it is said that, on firing a mixture of
common and inflammable air by electricity in a close copper vessel
holding about three pints, a loss of weight was always perceived, on
an average about two grains, though the vessel was stopped in such a
manner that no air could escape by the explosion. It is also related,
that on repeating the experiment in glass vessels, the inside of the
glass, though clean and dry before, immediately became dewy; which
confirmed an opinion he had long entertained, that common air deposits
its moisture by phlogistication. As the latter experiment seemed likely
to throw great light on the subject I had in view, I thought it well
worth examining more closely. The first experiment also, if there was
no mistake in it, would be very extraordinary and curious; but it did
not succeed with me; for though the vessel I used held more than Mr.
Warltire’s, namely, 24,000 grains of water, and though the experiment
was repeated several times with different proportions of common and
inflammable air, I could never perceive a loss of weight of more than
one-fifth of a grain, and commonly none at all. It must be observed,
however, that though there were some of the experiments in which it
seemed to diminish a little in weight, there were none in which it
increased.
In all the experiments, the inside of the glass globe became dewy,
as observed by Mr. Warltire; but not the least sooty matter could be
perceived. Care was taken in all of them to find how much the air was
diminished by the explosion, and to observe its test. The result is as
follows, the bulk of the inflammable air being expressed in decimals of
the common air:
------+-----------+----------+-------------+------------+--------
| | |Air Remaining|Test of this|
Common|Inflammable|Diminution| after the | Air in the |Standard
Air | Air | | Explosion |First Method|
------+-----------+----------+-------------+------------+--------
1 | 1.241 | .686 | 1.555 | .055 | .0
| 1.955 | .642 | 1.423 | .063 | .0
| .706 | .647 | 1.059 | .066 | .0
| .423 | .612 | .811 | .097 | .03
| .331 | .476 | .855 | .339 | .27
| .206 | .294 | .912 | .648 | .58
------+-----------+----------+-------------+------------+---------
Public-domain text, read in full here on John Shaqi.
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