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

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Chapter 3<br />

In-cylin<strong>de</strong>r volume during compression is reported in the figure 3.10. The volume is<br />

<strong>de</strong>termined thanks to a <strong>la</strong>ser piston positioning sensor being the compression time<br />

estimated on 44 ms. The piston velocity is comprised between 0 and 15 m/s, and it is<br />

around 9.5 m/s on average. In or<strong>de</strong>r to avoid measurements uncertainties, another<br />

<strong>la</strong>ser piston position sensor was p<strong>la</strong>ced at TDC and the pressure and piston position<br />

signals synchronized.<br />

The same procedure was followed when working with compression-expansion strokes<br />

without <strong>combustion</strong> (motored) being the pressure trace repetition verified in the figure<br />

3.11.<br />

30<br />

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

Pressure (bar)<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

Shot 1<br />

Shot 2<br />

Shot 3<br />

90 100 110 120 130 140 150 160 170 180<br />

Time (ms)<br />

Figure 3.11 - Typical pressure trace for compression expansion of stoichiometric downdraft<br />

syngas-air mixture in a RCM. Initial Conditions: P i = 1.0 bar; T i = 293 K.<br />

A very good repetition of signals was found during compression expansion experiments<br />

being the maximum difference between peak pressures around 0.4 bar (27 bar on<br />

average) from one experiment to another. Notice the higher pressure peak (>2.0 bar,<br />

8%) of the compression expansion strokes compared with single compression stroke of<br />

the figure 3.9. To exp<strong>la</strong>in this difference the average piston disp<strong>la</strong>cement without<br />

<strong>combustion</strong> during the compression stroke for both working mo<strong>de</strong>s are shown in the<br />

figure 3.12.<br />

75

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