On the Effectiveness of Various Modes of Detonation Or Combustion
On the Effectiveness of Various Modes of Detonation Or Combustion
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And 2980°K. A shock m. Oves into the quiet air raising the pressure to 2. 84 atm. And accelerating the air to a velocity of •815 c . Consequently, the rarefaction wave which follows the detonation is stronger than that occurring in case DI, since it has to accelerate the burnt gas to the velocity . 815 c and to cause the pressure to drop from 17. 96 atm. To 2. 84 atm. When the detonation arrives at the closed end, at t = . 16 t, it is reflected as a shock through which the pressure rises from 1...7. 96 atm. To 60. 90 atm. And the temperature from 2980° to 3675°K. The rarefaction wave following the detonation is traversed by the reflected shock and then is reflected at the closed end. During this reflection process which takes place 19 from t = . 16 t to t = . 74 t, the pressure at the closed o o' ^ end drops from 60. 90 atm. (see Table 3) to 2. 2 atm. And the temiperature from 3675°K to 2210°K. The shock and the rare- faction wave, reflected from the closed end, will eventually meet the interface between air and burnt gas.
What to read after On the Effectiveness of Various Modes of Detonation Or Combustion?
You can find similar books in the "Read Also" column, or choose other free books by Charles Deprima to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
And 2980°K. A shock m. Oves into the quiet air raising the pressure to 2. 84 atm. And accelerating the air to a velocity of •815 c . Consequently, the rarefaction wave which follows the detonation is stronger than that occurring in case DI, since it has to accelerate the burnt gas to the velocity . 815 c and to cause the pressure to drop from 17. 96 atm. To 2. 84 atm. When the detonation arrives at the closed end, at t = . 16 t, it is reflected as a shock through which the pressure rises from 1...7. 96 atm. To 60. 90 atm. And the temperature from 2980° to 3675°K. The rarefaction wave following the detonation is traversed by the reflected shock and then is reflected at the closed end. During this reflection process which takes place 19 from t = . 16 t to t = . 74 t, the pressure at the closed o o' ^ end drops from 60. 90 atm. (see Table 3) to 2. 2 atm. And the temiperature from 3675°K to 2210°K. The shock and the rare- faction wave, reflected from the closed end, will eventually meet the interface between air and burnt gas.
What to read after On the Effectiveness of Various Modes of Detonation Or Combustion?
You can find similar books in the "Read Also" column, or choose other free books by Charles Deprima to read onlineMoreLess
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