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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 />

Eng<strong>in</strong>e Size<br />

Eng<strong>in</strong>es <strong>of</strong> <strong>si</strong>milar de<strong>si</strong>gn generally run at the same piston speed. This is achieved by<br />

us<strong>in</strong>g small eng<strong>in</strong>es hav<strong>in</strong>g larger RPM and larger eng<strong>in</strong>es hav<strong>in</strong>g smaller RPM. Due<br />

to same piston speed, the <strong>in</strong>let velocity, degree <strong>of</strong> turbulence and flame speed are<br />

nearly same <strong>in</strong> <strong>si</strong>milar eng<strong>in</strong>es regardless <strong>of</strong> the <strong>si</strong>ze. However, <strong>in</strong> small eng<strong>in</strong>es the<br />

flame travel is small and <strong>in</strong> large eng<strong>in</strong>es large. Therefore, if the eng<strong>in</strong>e <strong>si</strong>ze is doubled<br />

the time required for propagation <strong>of</strong> flame through <strong>combustion</strong> space is also doubled.<br />

But with lower RPM <strong>of</strong> large eng<strong>in</strong>es the time for flame propagation <strong>in</strong> terms <strong>of</strong> crank<br />

would be nearly same as <strong>in</strong> small eng<strong>in</strong>es. In other words, the number <strong>of</strong> crank degrees<br />

required for flame travel will be about the same irrespective <strong>of</strong> eng<strong>in</strong>e <strong>si</strong>ze provided the<br />

eng<strong>in</strong>es are <strong>si</strong>milar.<br />

5. . Other Factors. Among the other factors, the factors which <strong>in</strong>crease the flame speed<br />

are supercharg<strong>in</strong>g <strong>of</strong> the eng<strong>in</strong>e, spark tim<strong>in</strong>g and re<strong>si</strong>dual gases left <strong>in</strong> the eng<strong>in</strong>e at<br />

the end <strong>of</strong> exhaust stroke. The air humidity also affects the flame velocity but its exact<br />

effect is not known. Anyhow, its effect is not large compared with A :F ratio and<br />

turbulence.<br />

PHENOMENON OF KNOCKING IN SI<br />

ENGINE<br />

(VTU July06/Jan 07)<br />

Knock<strong>in</strong>g is due to auto ignition <strong>of</strong> end<br />

portion <strong>of</strong> unburned charge<br />

<strong>in</strong><br />

<strong>combustion</strong> chamber. As the normal<br />

flame proceeds across the chamber,<br />

pressure and temperature <strong>of</strong> unburned<br />

charge <strong>in</strong>crease due to compres<strong>si</strong>on by<br />

burned portion <strong>of</strong> charge. This unburned<br />

compressed charge may auto ignite<br />

under certa<strong>in</strong> temperature condition and<br />

release the energy at a very rapid rate<br />

compared to normal <strong>combustion</strong><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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