Читать книгу Fundamentals of Heat Engines - Jamil Ghojel - Страница 54

1.3.5.4 Isentropic Flow

Оглавление

Examples include flow in ducts, nozzles, and diffusers without heat transfer and work being done. Knowing , where a is the speed of sound and Ma is the Mach number at the inlet, and rewriting Eq. (1.64) as


we obtain


Also,


Combining the last two equations, we get

(1.67)

From Eqs. (1.48) and (1.67)

(1.68)

The pressure ratio for Ma = 1 at γ = 1.4 is equal to 1.893. This is the critical pressure ratio for air. To achieve supersonic flow, the stagnation pressure needs to be such that pt > 1.893p.

Fundamentals of Heat Engines

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