Chapter 22
Unsteady Shock Wave, Contact Surface, and Wave Reflections
22.1. The shock wave equations and relations
We examine the problem of a shock wave (Ω) propagating parallel to the velocity of the upstream fluid in a fixed reference frame (A) (see Figure 22.1). We denote with D the propagation velocity of the shock wave in relation to the upstream fluid counted positive upstream: D is called the shock wave celerity.
The absolute velocity of the wave in the reference frame (A) is:
(since the flow is one-dimensional, we omit the vector sign above V1). The velocity V1 undergoes a discontinuity across (Ω) to take a value V2 and we write:
The quantity w = V2 – V1 represents the velocity difference experienced by the fluid across the shock (Ω). To make the shock wave steady, we consider a reference frame (R) moving with the velocity of the shock; i.e. V1 + D (see Figure 22.2). In (R), the upstream flow (1) encounters the shock wave with a velocity:
and becomes a state (2) with the velocity in (R):
Get Handbook of Compressible Aerodynamics now with the O’Reilly learning platform.
O’Reilly members experience books, live events, courses curated by job role, and more from O’Reilly and nearly 200 top publishers.