Scientific American Supplement, No. 508, September 26, 1885Various
Science
Scientific American Supplement, No. 508, September 26, 1885
Various
Science -- Periodicals
The specific heat of air at constant pressure has been proved by the
experiments of Regnault to be 0.2378, or something less than
one-fourth of that of water--a result arrived at by Rankine from
totally different data. In the case we have taken, there have been
expended 500 x 0.2378, or (say) 118.9[theta] to produce 26,450 f.p.
Each unit has therefore produced (26,450 / 118.0) = 222.5 f.p.,
instead of 772 f.p., which would have been rendered if every unit had
been converted into power. We therefore conclude that (222.5 / 772) = 29
per cent. of the total heat has been converted. The residue, or 71 per
cent., remains unchanged as heat, and may be partly saved by a
regenerator, or applied to other purposes for which a moderate heat is
required.
The quantity of heat necessary to raise the heat of air at a constant
volume is only 71 per cent. of that required to raise to the same
temperature the same weight of air under constant pressure. This is
exactly the result which Laplace arrived at from observations on the
velocity of sound, and may be stated thus--
Specific Foot- Per
heat. pounds. cent.
Kp = 1 lb. of air at constant pressure 0.2378 x 772 = 183.5 = 100
Kv = 1 lb. of air at constant volume 0.1688 x 772 = 130.3 = 71
------ --- ----- ---
Difference, being heat converted into power 0.0690 x 772 = 53.2 = 29
Or, in a hot-air engine without regeneration, the maximum effect of 1
lb. of air heated 1 deg. Fahr. would be 53.2 f.p. The quantity of heat
Ky necessary to heat air under constant volume is to Kv, or that
necessary to heat it under constant pressure, as 71:100, or as
1:1.408, or very nearly as 1:SQRT(2)--a result which was arrived
at by Masson from theoretical considerations. The 71 per cent.
escaping as heat may be utilized in place of other fuel; and with the
first hot-air engine I ever saw, it was employed for drying blocks of
wood. In the same way, the unconverted heat of the exhaust steam from
a high-pressure engine, or the heated gases and water passing away
from a gas-engine, may be employed.
[Illustration]
Public-domain text, read in full here on John Shaqi.
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