The Steam Injector
A theoretical and practical treatise on the design and operation of injectors and on the flow of fluids through and the design of nozzles.
Forfatter: V. A. B. Hughes
År: 1912
Forlag: The Technical Publishing Company Limited
Sted: London
Sider: 145
UDK: 621.176
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88
THE STEAM INJECTOR.
Generally speaking, the most efficient injector is one
whiøh, when delivering- i nto a boiler under a certain pres-
sure, passes the greatest ratio by weight of water to steam.
If, hcwever, we are oonsidering an injector from the point
of view of the temperature of the feed water it can deal
witih when the steam is at a certain pressure, the most
efficiient injector is one capa/ble of taking the hottest feed
water with the steam at thait pressure.
If the nunaber of heat units contained in 1 Ib. of the steam
entering the injector be known, also the temperatures of
the feed or supply water and of the delivery jet, then
with tx + Lj denoting the total heat contained in 1 Ib. of
the ,steam, ti the temperature of the feed water, t3 the
temperature of the delivery, and W the weight in Ibs. of
water per Ib. of steam,
Gain of heat by feed water = W (^3 - t.,).
Loss of heat of 1 Ib. of steam = t1 + lx - t3.
Heat equivalent of the kinetic energy of the jet leaving
the injector
= (W + 1) x V3
2 <7 x 778
where V — velocity of delivery jet in feet per second.
If the extre-mely small amount of heat energy repie-
sentied by the kinetic energy of the entering feed water
be neglected, also the loss of heat due to radiation from
the injector, then :—
Loss of heat Heat equivalent of kinetic . , „ ,
by steam = energy of delivery jet + fee<i
We have already seen that the heat equivalent of the
kinetic energy of the delivery jet is very small, and it can
be safely neglected without materially affecting the results.
The equation then becomes:-—-
tx + Lx - t3 = W (t3 -
i.e., AV = .... (xxviii.)