Review Article

Numerical Simulation of Unsteady Compressible Flow in Convergent Channel: Pressure Spectral Analysis

Figure 5

The unsteady numerical solution of the airflow in 𝐷 1 𝑓 = 1 0 0 Hz, 𝑀 = 0 . 0 1 2 , R e = 4 4 8 1 , 𝑝 2 = 1 / 𝜅 , and 4 5 0 × 1 0 0 cells. Data computed during the fourth oscillation cycle. Results are mapped by isolines of velocity ratio and by streamlines.
545120.fig.005a
(a) 𝑡 = 3 0 m s , 𝑔 = 1 . 6 m m , 𝑀 m a x = 0 . 1 5 9 ( 5 4 . 5 m s 1 )
545120.fig.005b
(b) 𝑡 = 3 2 . 5 m s , 𝑔 = 0 . 4 m m , 𝑀 m a x = 0 . 2 3 6 ( 8 0 . 9 m s 1 )
545120.fig.005c
(c) 𝑡 = 3 5 m s , 𝑔 = 1 . 6 m m , 𝑀 m a x = 0 . 3 7 0 ( 1 2 6 . 9 m s 1 )
545120.fig.005d
(d) 𝑡 = 3 7 . 5 m s , 𝑔 = 2 . 8 m m , 𝑀 m a x = 0 . 0 9 7 ( 3 3 . 3 m s 1 )
545120.fig.005e
(e) 𝑡 = 4 0 ms, 𝑔 = 1 . 6 m m , 𝑀 m a x = 0 . 1 6 2 ( 5 5 . 6 m s 1 )