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Handbook of Turbomachinery Second Edition Revised - Ventech!

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cycle known as staged combustion (some refer to it as a topping cycle).<br />

Third, the engine was to be capable <strong>of</strong> throttling, or varying its thrust to<br />

support the ascent trajectory requirements <strong>of</strong> the Space Shuttle vehicle.<br />

From a design thrust level <strong>of</strong> (appropriately) 100% rated power (referred to<br />

as RPL), the engine was to be capable <strong>of</strong> reduction in thrust to a minimum<br />

<strong>of</strong> 65% <strong>of</strong> design. This is referred to as minimum power level, or MPL. Also,<br />

thrust was to be capable <strong>of</strong> increasing to 109% <strong>of</strong> the design thrust. This<br />

high thrust was to be used for emergency conditions. As such, it was referred<br />

to as emergency power level, or EPL. Thrust variations were to be<br />

controllable to increments <strong>of</strong> 1%. Another notable feature <strong>of</strong> the original<br />

engine design was the requirement for a variable mixture ratio, or ratio <strong>of</strong><br />

oxidizer to fuel being consumed by the engine. This ratio was to be variable<br />

from 5:1 to 7:1 as commanded from the Shuttle orbiter. This feature was to<br />

be an attempt to ensure simultaneous depletion <strong>of</strong> both fuel and oxidizer<br />

tanks. This combination <strong>of</strong> operating conditions placed demands on the<br />

turbomachinery systems that remain unmatched 20 years later.<br />

Before proceeding further, a short comparison <strong>of</strong> the SSME operating<br />

cycle with those <strong>of</strong> its ancestors would be helpful. The Thor engine and its<br />

descendants, along with the F-1 and J-2 engines, shared a common<br />

thermodynamic cycle, the gas generator cycle. In this cycle, propellants<br />

from the vehicle tanks reach the turbopump inlets under tank pressure.<br />

Turbopump discharge ducting routes most <strong>of</strong> the fuel and oxidizer to the<br />

thrust chamber inlet manifolds. A small amount <strong>of</strong> both propellants,<br />

typically 2–3% <strong>of</strong> the total flow, is carried from the pump outlets to another<br />

combustor, referred to as a gas generator. Usually quite small in<br />

comparison to the main thrust chamber, the gas generator burns its<br />

propellants at a mixture ratio to produce gas (usually fuel rich) to serve as<br />

turbine drive fluid. Typically, these gases are in the 1000 to 1700 8F range.<br />

Although it would certainly be possible to create turbine drive gas that is<br />

oxidizer-rich rather than fuel-rich, the generally adverse chemistry<br />

associated with this situation normally renders fuel-rich gas a better choice.<br />

To this author’s knowledge, oxidizer-rich gas generators have not been<br />

employed in any production engines produced in the United States,<br />

although they have been (and still are) in use by other countries. Upon exit<br />

from the gas generator, the drive gas is transported to the inlet manifold <strong>of</strong><br />

the turbine(s). Following expansion through whatever turbine arrangement<br />

has been provided, the gas is typically either dumped to atmosphere<br />

through an exhaust duct or is transported to the divergent section <strong>of</strong> the<br />

engine exhaust nozzle, where it is injected into the supersonic flow stream.<br />

Being relatively cool, this gas can provide what is referred to as dump<br />

cooling <strong>of</strong> some portion <strong>of</strong> the nozzle divergent section. Incidentally, if drive<br />

gas is simply ducted overboard, a restricting orifice is normally placed in<br />

Copyright © 2003 Marcel Dekker, Inc.

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