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

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Numerical simu<strong>la</strong>tion of a syngas-fuelled engine<br />

mixture due to wall interaction. The entire flowchart of the <strong>de</strong>veloped co<strong>de</strong> is shown in<br />

figure 6.2.<br />

It requires as input data the engine geometric characteristics, engine speed, fuel–air<br />

equivalence ratio, <strong>combustion</strong> chamber walls temperature, compression ratio, ignition<br />

<strong>de</strong><strong>la</strong>y, and temperature and pressure of charge at IVC event. It is assumed that during<br />

compression the cylin<strong>de</strong>r content, consisting of air–fuel mixture and any residual<br />

gases, comprises one zone. From the start of <strong>combustion</strong>, multiple burned zones<br />

(whose number is user-<strong>de</strong>fined) are sequentially generated, with the <strong>la</strong>test-generated<br />

burned zone being separated from the unburned zone by an infinitesimally thin f<strong>la</strong>me<br />

front. The multi-zone approach is retained throughout the expansion phase, i.e. from<br />

the end of <strong>combustion</strong> until the EVO.<br />

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

All zones consi<strong>de</strong>red are assigned spatially uniform pressure, temperature and<br />

composition at any instant of time. During all phases, the pressure is uniform<br />

throughout the cylin<strong>de</strong>r at any instant of time. It is noted that the mo<strong>de</strong>l, being zerodimensional<br />

in nature, does not predict geometrically the actual position of the f<strong>la</strong>me<br />

front and the various zones insi<strong>de</strong> the cylin<strong>de</strong>r. Rather, simu<strong>la</strong>tion follows purely the<br />

thermodynamic approach.<br />

176

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