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

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Experimental set ups and diagnostics<br />

schlieren visualizations used for the <strong>de</strong>termination of the burning velocity at constant<br />

pressure. Each one is <strong>de</strong>scribed in the next sub-sections.<br />

3.2.1 F<strong>la</strong>mmability limits<br />

The f<strong>la</strong>mmability limit is a most wi<strong>de</strong>ly used in<strong>de</strong>x for representing the f<strong>la</strong>mmability<br />

characteristics of gases. In accordance with generally accepted usage, the f<strong>la</strong>mmability<br />

limits are known as those regions of fuel–air ratio within which f<strong>la</strong>me propagation can<br />

be possible and beyond which f<strong>la</strong>me cannot propagate. And there are two distinct<br />

separate f<strong>la</strong>mmability limits for the fuel–air mixture, namely, the leanest fuel-limit up to<br />

which the f<strong>la</strong>me can propagate is termed as lower f<strong>la</strong>mmability limit (LFL), and the<br />

richest limit is called as upper f<strong>la</strong>mmability limit (UFL).<br />

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

There are several criteria to <strong>de</strong>termine the f<strong>la</strong>mmability limits. A successful attempt can<br />

be <strong>de</strong>termined by one or a combination of the following criteria: (1) inspection of the<br />

visualization of the f<strong>la</strong>me kernel produced by the spark, namely visual criterion, and (2)<br />

measurements of pressure or temperature histories in the vessel and appropriate<br />

pressure or temperature rise criteria can be used to <strong>de</strong>signate f<strong>la</strong>mmability rather than<br />

the purely visual observation of f<strong>la</strong>me <strong>de</strong>velopment. As we know, a successful ignition<br />

would induce a rapid pressure increase and temperature rise within a short time, as<br />

well as produce a propagating f<strong>la</strong>me front that could be readily observed.<br />

Previous gas f<strong>la</strong>mmability limit data were obtained mainly in f<strong>la</strong>mmability tubes, in<br />

those tests, a gas mixture in a vertical tube was ignited and f<strong>la</strong>me propagation was<br />

inspected by a visual criterion. The wall quenching has a significant effect on the<br />

f<strong>la</strong>mmability measurement in f<strong>la</strong>mmability tube. The <strong>la</strong>rger size of <strong>combustion</strong> chamber<br />

can minimize wall effects and can allow for the potential use of stronger igniters to<br />

ensure the absence of ignition limitations, so most of the f<strong>la</strong>mmability measurements<br />

are conducted in closed chambers recently (Liekhus et al., 2000).<br />

For safety reasons, to prevent acci<strong>de</strong>ntal explosions during chemical processes and to<br />

c<strong>la</strong>ssify gas and gas mixtures for storage and transport, there are standards for the<br />

<strong>de</strong>termination of the explosion limit in atmospheric conditions that can be found in<br />

Schro<strong>de</strong>r and Molnarne, (2005). In general, the explosion limits are affected by the<br />

apparatus and material parameters. The most important are:<br />

- F<strong>la</strong>mmable mixture composition, type and amount of inert gas, fuel and<br />

oxidizer;<br />

- Initial pressure and initial temperature;<br />

68

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