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FIRST STEPS TOWARD SPACE - Smithsonian Institution Libraries

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134 SMITHSONIAN ANNALS OF FLIGHT<br />

A<br />

FICURE 1.—Model B rocket. From Oberth, Wege zur Raumschiffahrt,<br />

1929.<br />

they provide a greater specific impulse. From the<br />

requirement for a lightweight rocket structure came<br />

the realization that ceramic materials could not be<br />

used for rockets with liquid propellants. In these<br />

rockets the combustion chamber has to be light in<br />

weight and must have a thin wall, and the walls<br />

have to be kept cool by flowing the fuel around<br />

them. With this method, regenerative cooling is<br />

accomplished. The pressure in the combustion<br />

chamber must not be too low, otherwise the gas<br />

exhausts at too low a velocity. The tanks, however,<br />

should be under low pressure so that the walls do<br />

not have to be too thick. From this consideration<br />

the need for fuel pumps resulted. By the way, the<br />

paper also contained a relatively simple mathematical<br />

criterion for determining the advantage or<br />

disadvantage of using a device which increased the<br />

exhaust velocity but diminished the mass ratio of<br />

empty rocket to filled rocket.<br />

In spite of regenerative cooling I did not want<br />

the temperature of the combustion chamber to be<br />

too high, especially because the titanium and vanadium-steel<br />

alloys of today were not known at that<br />

time. A means of decreasing the temperature of the<br />

combustion chamber without reducing the exhaust<br />

velocity is available by adding another element to<br />

the propellant which does not burn but only evaporates,<br />

thus creating a specifically light vapor. When<br />

combining hydrogen and oxygen, for example, the<br />

excess of hydrogen creates that effect (Esnault-<br />

Pelterie called it the "Oberth-effect").<br />

In this way I had, in the 1920s, experimentally<br />

achieved a propulsion system which reached exhaust<br />

speeds of 3,900 m/sec to 4,0000 m/sec. I used<br />

the propellants, however, in their gaseous state<br />

because in Transylvania I could neither obtain<br />

them in liquid form nor find means to liquefy them.<br />

I wrote about this to some friends in Vienna;<br />

whereupon a professor of the Vienna Technical<br />

University answered that I must be a fraud. He had<br />

calculated that hydrogen and oxygen, even when<br />

used in their stoichiometrically correct proportion,<br />

could not provide more than 3,200 m/sec because of<br />

dissociation. However, he did not think of the fact<br />

that dissociation is practically zero because of the<br />

excess of hydrogen and the low temperature. Pure<br />

hydrogen can be lighter and achieve a greater exhaust<br />

velocity at low temperature than dissociated<br />

or even undissociated H20 vapor at high temperature.<br />

Today the Americans use H2 and 02 in their

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