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

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Chapter 3<br />

nair<br />

4.76( f φ)<br />

P = P =<br />

P<br />

n a + b + c + d + e + 4.76 ( f φ)<br />

air m m<br />

m<br />

(3.7)<br />

Where φ is the equivalence ratio. The syngas-air mixture was prepared within the<br />

<strong>combustion</strong> chamber. The initial conditions were strictly controlled in the experiments to<br />

realize the same initial pressure and temperature. For avoiding the influence of wall<br />

temperature on mixture temperature, an enough interval between two experiments is<br />

set, providing enough time for wall to cool down to the room temperature.<br />

3.1.2 Rectangu<strong>la</strong>r chamber<br />

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

The static rectangu<strong>la</strong>r <strong>combustion</strong> chamber shown in figure 3.1 has two transparent<br />

si<strong>de</strong>s in ordinary g<strong>la</strong>ss (BK7) providing <strong>la</strong>rge enough optical access to schlieren<br />

photography. The insi<strong>de</strong> size of the rectangu<strong>la</strong>r chamber is 70 mm width, 58 mm length<br />

and 120 mm height. The material of the chamber is duraluminum (AU4G).<br />

Electro<strong>de</strong><br />

Injector<br />

Exhaust<br />

valve<br />

Figure 3.1 – Rectangu<strong>la</strong>r <strong>combustion</strong> chamber<br />

The pressure is recor<strong>de</strong>d by a dynamic sensor Kistler 601A installed in the bottom si<strong>de</strong><br />

of the chamber with resolution of 0.1 mbar. The chamber has an admission/exhaustion<br />

valve for mixture admission and <strong>combustion</strong> gases exhaustion.<br />

The Synerjet-Orbital injector installed on the top surface of the chamber was conceived<br />

by Malheiro, (2002). This chamber is able to embrace the ignition electro<strong>de</strong> in three<br />

different positions. This type of electro<strong>de</strong>s conception allows the possibility to change<br />

the spark position in the <strong>combustion</strong> chamber and also allows the variation of the<br />

electro<strong>de</strong> gap. Such as Malheiro, (2002), the electro<strong>de</strong> gap employed in the<br />

experiments was 2.0 mm.<br />

63

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