THESE de DOCTORAT - cerfacs
THESE de DOCTORAT - cerfacs
THESE de DOCTORAT - cerfacs
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118 Chapter 6: Boundary conditions for low Mach number acoustic co<strong>de</strong>s<br />
values of R computed by SNozzle match the values of R given analytically when the wave<br />
length is extremely large compared to L (Ω ≈ 0). This is shown in Figs 6.15 and 6.16.<br />
" c<br />
= 2<br />
" c<br />
= 4<br />
9<br />
8<br />
¯M 2 =0.025<br />
¯M 2 =0.05<br />
¯M 2 =0.1<br />
9<br />
8<br />
¯M 2 =0.025<br />
¯M 2 =0.05<br />
¯M 2 =0.1<br />
7<br />
7<br />
Module of R<br />
6<br />
5<br />
4<br />
Module of R<br />
6<br />
5<br />
4<br />
3<br />
3<br />
2<br />
2<br />
1<br />
1<br />
0 0.05 0.1<br />
!<br />
0 0.05 0.1<br />
!<br />
(a)<br />
(b)<br />
Figure 6.15: Modulus of the Reflection Coefficient. Lines represent SNozzle solutions. Symbols<br />
(◦) stands for Analytical results<br />
.<br />
From Fig. 6.15 it is observed that, for a given ¯π c , lower values of ¯M 2 lead to smaller values<br />
of |R|. For high values of ¯π c , the magnitu<strong>de</strong> or the reflection coefficient increases significantly<br />
mainly for low forcing frequencies. It should be clear then that the inclusion of an enthalpy<br />
jump is crucial for the estimation of acoustic boundaries to impose at the edge of a combustion<br />
chamber within an aeronautical engine.