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FIRST STEPS TOWARD SPACE - Smithsonian Institution Libraries

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218 SMITHSONIAN ANNALS OF FLIGHT<br />

Vienna—because his goal was to develop an aircraft<br />

engine—limited his efforts to testing propulsion<br />

units, but he proceeded very systematically and<br />

obtained valuable test data.<br />

Though Sanger started his tests later than the<br />

German group and worked mainly by himself, he<br />

was in a more advantageous position: from the<br />

very beginning, because of his different objective,<br />

he devoted more attention to the problem of cooling<br />

his rocket engine than the German group did.<br />

The latter, when not simply relying on the heat<br />

capacity of the combustion chamber walls, placed<br />

the engine into a container filled with a stagnant<br />

coolant, although Oberth had already proposed in<br />

his book a regenerative cooling process. Since<br />

Sanger wanted to develop a rocket engine for a<br />

manned aircraft and not a ballistic projectile to be<br />

launched vertically, he had to build his engine so<br />

carefully and so safe that it would be reusable<br />

many times. Thus, he initially concentrated on the<br />

development of the engine itself, without facing<br />

the complex problems of producing a flightworthy<br />

overall system. Consequently, he could devote more<br />

attention to the so-called "braking tests" in a<br />

ground test facility than other researchers did who<br />

were interested in reporting as fast as possible on<br />

flight altitudes and ranges obtained by their ballistic<br />

rocket models. (He called these "braking tests" in<br />

analogy with tests of internal combustion engines,<br />

in which torque is braked and measured, whereas<br />

in his tests the thrust was being sustained and<br />

measured.) Sanger prepared his tests in a most<br />

systematic and logical way and, especially in studying<br />

cooling problems, took advantage of tapwater<br />

available from a stationary source. From the very<br />

beginning, Sanger's tests aimed at obtaining high<br />

exhaust velocities which are accompanied by high<br />

combustion temperatures and chamber wall stresses,<br />

whereas Oberth and his followers tried to achieve<br />

first of all simply a "functioning" of the rocket engine<br />

and artificially lowered the combustion temperatures<br />

by water injection.<br />

To aid in understanding the development approaches<br />

taken in the early German and Austrian<br />

rocket projects described herein, a systematic synopsis<br />

of possible and so far known cooling methods<br />

for rocket engines is being attempted. In principle,<br />

two methods can be distinguished for cooling<br />

rocket engine parts exposed to combustion gases—<br />

capacity (capacitance, or heat-soak) and dynamic<br />

cooling.<br />

Capacitance cooling is a static process whereby<br />

heat flowing from the combustion chamber is stored<br />

by the solid chamber walls and—if they are present—also<br />

by the walls of a cooling jacket surrounding<br />

the thrust chamber. The heat thus received is<br />

continually collected within the coolant material,<br />

but this method does not result in an equilibrium<br />

condition and is useful for a limited time only, i.e.,<br />

until the heat storage capacity is exhausted. A limit<br />

case of capacity cooling is represented by ablation<br />

cooling; here heat is dissipated by successive melting<br />

or subliming of a suitable protective layer<br />

(e.g., nylon, phenolic resin, or graphite) covering<br />

parts endangered by heat.<br />

The term dynamic cooling covers any method<br />

using conduction, convection, or radiation to dissipate<br />

from the endangered zone that amount of<br />

heat which cannot be stored by the combustion<br />

chamber walls. There are two ways to accomplish<br />

this:<br />

1. To minimize heat transfer from the combustion<br />

gas into the heated wall side either by reducing<br />

the temperature difference between both (high<br />

wall temperatures with refractory wall materials,<br />

artificial reduction of combustion temperature<br />

by water injection, etc.) or by influencing the<br />

boundary layer (coolant mist, optically reflective<br />

wall surfaces, electrical fields for sufficiently<br />

ionized combustion gases, etc.).<br />

2. To dissipate as Tapidly as possible the heat contained<br />

in the chamber wall by maximizing heat<br />

transfer from the cooled chamber-wall side into<br />

an adjoining suitable and efficiently ducted<br />

coolant.<br />

Gartmann proposed the terms "internal," and "external"<br />

cooling for these two methods.<br />

Film cooling, invented by Oberth and achieved<br />

by injecting water into the boundary layer, is an<br />

example of internal dynamic cooling. In the case of<br />

external dynamic cooling—where the amount of<br />

heat from the hot combustion gases, passing to and<br />

across the combustion chamber wall and then into a<br />

flowing coolant, is carried off with the coolant—a<br />

state of equilibrium can be obtained if the coolant<br />

can be ducted in such a way that the heat amount<br />

received by the heated chamber wall side equals

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