28.01.2013 Views

Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

Zienkiewicz O.C., Taylor R.L. Vol. 3. The finite - tiera.ru

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

292 Appendix A<br />

Again substituting the continuity equation into the above equation, we have the<br />

reduced form of the energy equation<br />

@E<br />

@t ‡ u @E<br />

j<br />

@x j<br />

1 @<br />

ÿ<br />

@xi k @T<br />

@x i<br />

‡ 1 @…ui p†<br />

ÿ<br />

@xi 1 @… ijuj† @xi …A:7†<br />

Some authors use Eqs. (A.1), (A.5) and (A.7) to study compressible ¯ow problems.<br />

However these non-conservative equations can result in multiple or incorrect solutions<br />

in certain cases. This is t<strong>ru</strong>e especially for high-speed compressible ¯ow problems with<br />

shocks. <strong>The</strong> reader should note that such non-conservative equations are not suitable<br />

for simulation of compressible ¯ow problems.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!