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THESE de DOCTORAT - cerfacs

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138 Chapter A: About the π ′ c = 0 assumption<br />

and<br />

¯π T h ′ t,1 ¯v θ,1 = h ′ t,2 ¯v θ,2<br />

(A.19)<br />

Summarizing, the fluctuation of the parameter π<br />

T ′ can be neglected if<br />

v ′ θ,1 = v′ θ,2 and ¯π T h ′ t,1 ¯v θ,1 = h ′ t,2 ¯v θ,2 (A.20)<br />

or<br />

v ′ θ,1<br />

= h′ t,1<br />

v θ,1 ¯ ¯h t,1<br />

or<br />

v ′ θ,2<br />

= h′ t,2<br />

v θ,2 ¯ ¯h t,2<br />

(A.21)<br />

The parameter π T is related to the total pressure ratio π c as π T<br />

variation of π c is written.<br />

= π c<br />

(γ−1)/γ . The fractional<br />

π<br />

T<br />

′ = γ − 1 π c<br />

′<br />

¯π T γ ¯π c<br />

(A.22)<br />

It is observed then that making π ′ T = 0 is equivalent to make π′ c = 0, which is a clear simplification<br />

for the <strong>de</strong>finition of the differential equation of momentum in SNozzle. In<strong>de</strong>ed, doing<br />

π ′ c = 0 means that p ′ t,2 /p′ t,1 = ¯π c

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