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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.

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