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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THE DELIVERY NOZZLE.
37
the initial pressure as zero. The diameters of the nozzle
at the different equidistant sections are as follows : —
Section 1 ................ Diameter 1 or unity.
„ 2 ................. „ 1-034.
.................
„ 3 ................. „ 1-074.
„ 4 .........................., 1-124,
„ 5 ................. „ 1-188.
„ 6 ................. „ 1-276.
„ ‘ ................ „ 1-411................
„ 8 ................. „ 1-673.
„ 9 ................. „ 4-152.
It will be seen that the rate of increase in the diameter
of the nozzle is very slow right up to section 8.
It is found in practice that if the jet contain any solid
matter, abrasion of the deliveiy nozzle takes place chiefiy
around the throat or first portion of the latter. It is usual
practice to make the d&livery nozzle of cylindrical form at
the throat for a length equal to the diameter of the
throat, as shown at fig. 19.
If the form of the nozzle be such as to cause a very sudden
increase in the pressure of the jet at a point near to the
throat of the nozzle where the velocity is high, the jet sets
up a strong abrading action on, and tends to groove, the
nozzle surface at that point. In this respect the form of
nozzle shown at fig. 18 is better than that shown at fig.
17. Towards the delivery end of the nozzle the velocity
of the jet is small, and wear is reduced to a minimum.
In most injectors the delivery nozzle has a plain, conical
throughway aperture, as this form of nozzl& lends itself to
economical manufacture. A nozzle of this type is illus-
trat&d at fig. 20, which also gives corresponding velocity
and pressure curves when the entering velocity is taken as
200 ft. and also as 100 ft. per s&cond. It will be seen that
with this type of nozzle there is at first a rapid rise and
then a slow rise of pressure which will result in the prcduc-
tion of eddying motions in the jet between the sections 1