Note On the Theory of Rocket Motors

Cover Note On the Theory of Rocket Motors
Note On the Theory of Rocket Motors
Kurt Otto Friedrichs
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)df + f dp + mdv = (p - p )df . X Vi x *Q' x x *x x F x *0 x This indicates that the maximum thrust occurs when the gas at the end cross-section has just expanded to atmospheric pressure; -5- the thrust is then solely due to momentum transport. (Malina does not mention this fact explicitly. ) Wnen the end cross-section is so large that the exit pressure would be below outside pressure according to the theory as explained, the assumptions on which this theory is based are no longer valid; a diff...erent flow pattern involving shocks will occur. Malina determines the thrust under the assumption of a straight shock; the resulting change accounts for the break in the indicated graph.
Malina considers as an example a case with 2c. = 100, T = 11, 100°F. R = . 0658 B. T . U . /lb. /°F. , y = 1. 2, and finds that the maximum thrust is obtained when -g— - 11. 85, 1 t i. E. When the exit diameter is 3. 4-4 times the throat diameter.
The maximum thrust is given by F Ve = 13. 6, i. E. The thrust is 13.


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