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Handbook of Turbomachinery Second Edition Revised - Ventech!

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using hydrocarbon fuel combustion products have suffered progressive<br />

coking <strong>of</strong> the turbine nozzles. This gradual reduction in nozzle flow area<br />

resulted in decreasing turbine performance. To avoid this, the turbine inlet<br />

temperature was adjusted to move out <strong>of</strong> the range that accentuated the<br />

coking problem. Ironically, one production turbine had its inlet temperature<br />

lowered, while another responded favorably only with increased inlet<br />

temperature. Finally, a brief mention <strong>of</strong> the working fluid chemical<br />

properties is worthwhile. In the range <strong>of</strong> turbine inlet temperatures typically<br />

specified (800–1,700 8F is representative), the mixture ratio <strong>of</strong> oxidizer to<br />

fuel required is quite heavily biased by combustion system standards. This<br />

could, <strong>of</strong> course, be accomplished by biasing toward either excess fuel or<br />

excess oxidizer. Almost without exception, fuel-rich combustion products<br />

are specified for the working fluid <strong>of</strong> rocket turbines. There are two main<br />

reasons for this: first, the chemistry <strong>of</strong> fuel-rich gases, is typically favorable<br />

while that <strong>of</strong> oxidizer-rich gases can be quite adverse; and second, turbine<br />

mass flow requirements are normally lower with fuel-rich gases since they<br />

tend to have lower molecular weight than equivalent oxidizer-rich gas. It<br />

should be noted, however, that these conditions scarcely prohibit the use <strong>of</strong><br />

oxidizer-rich gases for turbine drive with proper attention to detail. Several<br />

engines operating with this type <strong>of</strong> turbine working fluid have been in use in<br />

other countries for many years. These engines have been developed to a high<br />

degree <strong>of</strong> refinement.<br />

Engines that operate on the expander cycle typically use the engine’s<br />

fuel (and/or oxidizer) heated in the combustion chamber cooling circuit for<br />

turbine drive. The success <strong>of</strong> this arrangement depends on the combustion<br />

chamber coolant fluid undergoing an adequate enthalpy increase in the<br />

chamber cooling process to satisfy turbine energy requirements. For this<br />

reason, the successful operation <strong>of</strong> this cycle can be thought <strong>of</strong> as a<br />

significant technical accomplishment. Fluids used in this application to date<br />

include supercritical hydrogen and oxygen.<br />

Given the turbine working fluid and its properties, we next discuss<br />

specification <strong>of</strong> the turbine inlet and exit pressures. Monopropellant turbine<br />

drive cycles probably have the greatest flexibility in this area, since the<br />

turbine working fluid is contained in an independent system. In these<br />

applications, turbine inlet pressure is determined by the allowable<br />

monopropellant tank pressure, while accounting for the losses between<br />

the monopropellant tank and the turbine inlet. Also, since the turbine fluid<br />

is exhausted to atmosphere in this cycle, high turbine pressure ratios are<br />

possible. The most recent example <strong>of</strong> such a system in a production rocket<br />

engine in the United States is the Redstone engine, built by the Rocketdyne<br />

Division <strong>of</strong> Rockwell International (then North American Aviation Inc.).<br />

This system employed a two-row velocity-compounded impulse turbine<br />

Copyright © 2003 Marcel Dekker, Inc.

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