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It is evident that since the net energy release decreases with w a v e velocity increase, the kinetic energy change increases faster than the static enthalpy change. T h u s , while energy-releasing chemical reactions continue to exist, the overall strong detonation process eventually b e c o m e s endothermic. O n the basis of classical detonation theory, this data suggests that one-dimensional equilibrium strong detonations can be classified as a r e g i m e of w a v e velocity and mixture ratio for certain given initial t h e r m o d y n a m i c state conditions.

T h e role of turbulence i n the transition period w a s discussed by Martin (9)· The results are presented i n Table 4. No significant p r e s s u r e t r e n d w a s i n v e s t i g a t e d . Shock ignition, i n general, w a s more effective than spark ignition in producing normal detonation velocities. At l o w v a l u e s o f d i a p h r a g m p r e s s u r e r a t i o , t h e r e s u l t w a s s i m i l a r to that w i t h s p a r k i g n i t i o n , b u t a s t h e d i a p h r a g m pressure ratio w a s increased, the pressure ratio across the d e t o n a t i o n s d e c r e a s e d , u n t i l v e l o c i t i e s a n d p r e s s u r e ratios very near the Chapman-Jouguet values were recorded.

R . W h i t e : The Formation and Structure of Gaseous Detonation W a v e s . Seventh Symposium ( I n t e r n a t i o n a l ) o n C o m b u s t i o n , p p . 856-865· Butterworths S c i e n t i f i c P u b l i c a t i o n s , L o n d o n , 1959· 10 W . J o s t , T h . Just a n d H . G g . W a g n e r : Investigations of t h e R e a c t i o n Z o n e o f G a s e o u s D e t o n a t i o n s . Eighth Symp o s i u m ( I n t e r n a t i o n a l ) o n C o m b u s t i o n , I960 (in p r i n t ) . 11 K.

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