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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 />

6.3.2 RCM<br />

As shown in chapter 5, RCM simu<strong>la</strong>tes a single engine cycle and some adaptations to<br />

the mo<strong>de</strong>l presented above are nee<strong>de</strong>d in or<strong>de</strong>r to take into account the dynamic and<br />

geometrical specificness of the RCM. Three main aspects should be consi<strong>de</strong>red, the<br />

instantaneous volume, heat transfer and burning rate. Two distinctive cases are<br />

consi<strong>de</strong>red in the co<strong>de</strong>: single compression, and compression and expansion strokes.<br />

6.3.2.1 F<strong>la</strong>me propagation<br />

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

The f<strong>la</strong>me <strong>de</strong>velopment in the <strong>combustion</strong> chamber of a RCM was shown above for the<br />

compression and expansion strokes. In or<strong>de</strong>r two verify the assumption frequently used<br />

for engine <strong>combustion</strong> mo<strong>de</strong>ls, where the f<strong>la</strong>me area is a spherical f<strong>la</strong>me front<br />

truncated by the cylin<strong>de</strong>r walls and the piston, centered at the spark plug adopted in<br />

this work, the f<strong>la</strong>me images are used in an image treatment Mat<strong>la</strong>b co<strong>de</strong> <strong>de</strong>veloped by<br />

Strozzi, (2008), which allows visualizing the f<strong>la</strong>me contours.<br />

Figures 6.5 show the f<strong>la</strong>me contours in a RCM <strong>combustion</strong> chamber for downdraft<br />

syngas-air stoichiometric mixture. The window has 613×337 pixels with resolution of<br />

2.835 pixels/mm. The frequency of the each contour is kept to 1.4 KHz.<br />

Figure 6.5 - RCM f<strong>la</strong>me contours of stoichiometric downdraft syngas-air mixture with ignition at<br />

12.5 ms BTDC.<br />

The earlier stage of f<strong>la</strong>me kernel with influence of the spark plug was removed from the<br />

contours due to <strong>la</strong>ck of <strong>de</strong>finition. After around 5.0 ms (the duration of the spark), the<br />

f<strong>la</strong>me contours are well <strong>de</strong>fined and shows that the propagation is spherical. At this<br />

moment the piston is reaching TDC and the f<strong>la</strong>me shows a remarkable slow down due<br />

to piston <strong>de</strong>a<strong>de</strong>ning, which is felt on the pressure signal by a <strong>de</strong>creasing gradient. After<br />

TDC, the f<strong>la</strong>me contour shows to near double the disp<strong>la</strong>cement due to expansion.<br />

182

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