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Handbook of Turbomachinery Second Edition Revised - Ventech!

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exposure may be subjected to impingement by cryogenic air with<br />

unpredictable results. Finally, the unusually low fuel temperature creates<br />

an external heat leakage problem that is usually impossible to ignore. The<br />

result is that most liquid hydrogen propellant systems contain large amounts<br />

<strong>of</strong> thermal insulation, and sometimes protective shells to prevent damage to<br />

the insulation.<br />

Another problem unique to LH 2 concerns its low density. Since<br />

changes in head and pressure are proportional to each other by the<br />

reciprocal <strong>of</strong> the fluid density, lower-density fluids require higher developed<br />

heads to impart a given pressure rise. In the case <strong>of</strong> hydrogen near<br />

saturation conditions, head rises required to develop a given pressure rise<br />

from a pump are an order <strong>of</strong> magnitude higher than that required for denser<br />

propellants such as kerosene, liquid oxygen, and others. Pump designs for<br />

LH2 service, therefore, typically require comparatively large amounts <strong>of</strong><br />

input power, have near-maximum impeller tip speeds, and are <strong>of</strong>ten<br />

multistage machines.<br />

The Rocketdyne Division <strong>of</strong> North American Aviation was the builder<br />

<strong>of</strong> the J-2 engine under contract to NASA. As it happened, the company<br />

had already been engaged in the development <strong>of</strong> a liquid hydrogen pump for<br />

a nuclear rocket engine project not related to the J-2 program. The LH2<br />

pump, called the Mark 9, worked to performance requirements similar to<br />

those <strong>of</strong> the J-2. The Mark 9 was an axial-flow pump with six main stages,<br />

plus an inducer. Although not a common design for a rocket pump, the<br />

axial-flow configuration had advantages in weight, packaging, efficiency and<br />

was relatively easy to multistage. For these reasons, as well as the lack <strong>of</strong> a<br />

throttling requirement (the J-2 was a fixed-thrust engine), the J-2 fuel pump<br />

was designed to a configuration very much akin to the Mark 9, although a<br />

seventh main stage was added to provide satisfactory stall margin. This<br />

pump (known as the Mark 15-F) went on to see a great deal <strong>of</strong> operational<br />

service in the upper stages <strong>of</strong> the Saturn 1B and Saturn V vehicles.<br />

In the late 1960s, the U.S. government decided that the next large<br />

launch vehicle development effort would center around a reuseable vehicle<br />

to ferry astronauts and cargo to and from low earth orbit. This vehicle was<br />

to become the Space Transportation System (STS) or Space Shuttle, which<br />

is currently operating. The system went through many incarnations during<br />

definition, the details <strong>of</strong> which are beyond the scope <strong>of</strong> this text. When, in<br />

1972, the vehicle configuration was chosen, the resulting propulsion system<br />

requirements were unlike any previously stipulated. First, the STS’s main<br />

propulsion system (later named the Space Shuttle main engine, or SSME)<br />

was to use LOX/LH 2 propellants and operate at a chamber pressure <strong>of</strong><br />

3,000 psi. This was three times higher than the highest pressure production<br />

engine prior to it. <strong>Second</strong>, the engine was to operate on a thermodynamic<br />

Copyright © 2003 Marcel Dekker, Inc.

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