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Etude de la combustion de gaz de synthèse issus d'un processus de ...

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Experimental study of engine-like turbulent <strong>combustion</strong><br />

-5.0 ms -3.75 ms -2.5 ms -1.25 ms TDC<br />

1.25 ms 2.5 ms 3.75 ms 5.0 ms 6.25ms<br />

(a)<br />

-6.25 ms - 5.0 ms -3.75 ms -2.5 ms -1.25 ms<br />

tel-00623090, version 1 - 13 Sep 2011<br />

TDC 1.25 ms 2.5 ms 3.75 ms 5.0 ms<br />

(b)<br />

-12.5 ms -11.25 ms -10.0 ms -8.75 ms - 7.5 ms<br />

-6.25 ms - 5.0 ms - 3.75 ms -2.5 ms -1.25 ms<br />

TDC 1.25 ms 2.5 ms 3.75 ms<br />

(c)<br />

Figure 5.23- Direct visualization of stoichiometric methane-air f<strong>la</strong>me in a RCM for various<br />

Ignition timings. (a) 5 ms BTDC; (b) 7.5 ms BTDC; (c) 12.5 ms BTDC.<br />

Pictures of the initial phase of <strong>combustion</strong> show an initially quasi-spherical, re<strong>la</strong>tively<br />

smooth f<strong>la</strong>me kernel for syngas compositions and methane cases for the various<br />

ignition timings. The <strong>la</strong>minar behavior of the f<strong>la</strong>me remains longer time as the ignition is<br />

ma<strong>de</strong> far from TDC. In the case of ignition timing at 12.5 ms BTDC, the f<strong>la</strong>me kernel<br />

grows and experience f<strong>la</strong>ttening when piston is close to TDC position before the<br />

transition to turbulent <strong>combustion</strong>.<br />

Because the <strong>combustion</strong> continues in the expansion stroke, it is not possible to<br />

<strong>de</strong>termine from direct f<strong>la</strong>me visualizations of the <strong>combustion</strong> chamber the <strong>combustion</strong><br />

duration. However, estimation about the rapidity of the <strong>combustion</strong> can be ma<strong>de</strong> from<br />

figures 5.21-5.23. It is observed that the time at which the f<strong>la</strong>me occupies the entire<br />

chamber increases as the igniting timing increases for the whole fuels. This<br />

164

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