THESE de DOCTORAT - cerfacs
THESE de DOCTORAT - cerfacs
THESE de DOCTORAT - cerfacs
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
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