Слайд 2
![Chapter 4 Rayleigh Flow](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-1.jpg)
Слайд 3
![Effect of upstream Mach number on the flow](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-2.jpg)
Effect of upstream Mach number on the flow
Слайд 4
![Critical added heat is at Ma=1 Energy Energy eq. becomes](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-3.jpg)
Critical added heat is at Ma=1
Energy
Energy eq. becomes
Continuity
State 1 is constant
and 2 is an arbitrary point (variable state)
Слайд 5
![At the point of tangency of H-curve and Rayleigh line the Mach number ALWAYS equals one](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-4.jpg)
At the point of tangency of H-curve and Rayleigh line the
Mach number ALWAYS equals one
Слайд 6
![Effect of upstream Mach number on the flow](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-5.jpg)
Effect of upstream Mach number on the flow
Слайд 7
![Beyond the tangent H-curve](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-6.jpg)
Beyond the tangent H-curve
Слайд 8
![Subsonic inlet (state 1) with q>q* lower Rayleigh line](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-7.jpg)
Subsonic inlet (state 1) with q>q*
lower Rayleigh line
Слайд 9
![Supersonic inlet (state 1) with q>q* Shock wave](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-8.jpg)
Supersonic inlet (state 1) with q>q*
Shock wave
Слайд 10
![Chapter 4: Lecture Problems In Rayleigh flow, prove that the](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-9.jpg)
Chapter 4: Lecture Problems
In Rayleigh flow, prove that the point of
tangency of H-curve and Rayleigh line represents a sonic flow.
Stagnation pressure proof.
Слайд 11
![End of Chapter 4](/_ipx/f_webp&q_80&fit_contain&s_1440x1080/imagesDir/jpg/285652/slide-10.jpg)