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combustion process in si engines - National Institute of Technology

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INTERNAL COMBUSTION ENGINES (ELECTIVE) (ME667)<br />

SIXTH SEMESTER<br />

<strong>combustion</strong> <strong>process</strong> and (c→d) is an expan<strong>si</strong>on <strong>process</strong>. In an ideal cycle it can be<br />

seen from the diagram, the entire pressure rise dur<strong>in</strong>g <strong>combustion</strong> takes place at<br />

constant volume i.e., at TDC. However, <strong>in</strong> actual cycle this does not happen.<br />

RICHARD’S THEORY OF COMBUSTION.<br />

Sir Ricardo, known as father <strong>of</strong> eng<strong>in</strong>e research describes the <strong>combustion</strong> <strong>process</strong><br />

can be imag<strong>in</strong>ed as if it is develop<strong>in</strong>g <strong>in</strong> two stages:<br />

1. Growth and development <strong>of</strong> a self propagat<strong>in</strong>g nucleus flame. ( Ignition lag)<br />

2. Spread <strong>of</strong> flame through the <strong>combustion</strong> chamber<br />

THREE STAGE OF COMBUSTION (VTU July/Aug 05/Feb 06/July 06)<br />

Accord<strong>in</strong>g to Ricardo, There are three stages <strong>of</strong> <strong>combustion</strong> <strong>in</strong> SI Eng<strong>in</strong>e as shown<br />

1. Ignition lag stage<br />

2. Flame propagation stage<br />

3. After burn<strong>in</strong>g stage<br />

1. Ignition lag stage: There is a certa<strong>in</strong><br />

time <strong>in</strong>terval between <strong>in</strong>stant <strong>of</strong> spark<br />

and <strong>in</strong>stant where there e is a noticeable<br />

rise <strong>in</strong> pressure due to <strong>combustion</strong>.<br />

This time lag is called IGNITION LAG.<br />

Ignition lag is the time <strong>in</strong>terval <strong>in</strong> the <strong>process</strong> <strong>of</strong> chemical reaction dur<strong>in</strong>g which<br />

molecules get heated up to self ignition temperature , get ignited and produce a<br />

self propagat<strong>in</strong>g nucleus <strong>of</strong> flame. The ignition lag is generally expressed <strong>in</strong><br />

terms <strong>of</strong> crank angle (θ1). (<br />

The period <strong>of</strong> ignition lag is shown by path ab. Ignition<br />

lag is very small and lies between 0.00015 to 0.0002 seconds. An ignition lag <strong>of</strong><br />

0.002 seconds s corresponds to 35 deg crank rotation when the eng<strong>in</strong>e is runn<strong>in</strong>g<br />

at 3000 RPM. Angle <strong>of</strong> advance <strong>in</strong>crease with the speed. This is a chemical<br />

<strong>process</strong> depend<strong>in</strong>g upon the nature <strong>of</strong> fuel, temperature and pressure,<br />

proportions <strong>of</strong> exhaust gas and rate <strong>of</strong> oxidation or burn<strong>in</strong>g.<br />

Jagadeesha T, As<strong>si</strong>stant Pr<strong>of</strong>essor, Department <strong>of</strong> Mechanical Eng<strong>in</strong>eer<strong>in</strong>g, Adichunchanagiri <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong>, Chikmagalur

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