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Design and Simulation of Two Stroke Engines

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Chapter 4 - Combustion in <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

4.1.3 Effect <strong>of</strong> scavenging efficiency on flammability<br />

In Sec. 3.1.5 there is mention <strong>of</strong> the scavenging efficiency variation with scavenge ratio.<br />

As the engine load, or brake mean effective pressure, bmep, is varied by altering the throttle<br />

opening thereby producing changes in scavenge ratio, so too does the scavenging efficiency,<br />

SE, change. It will be observed from Fig. 3.10, even for the best design <strong>of</strong> two-stroke engines,<br />

that the scavenging efficiency varies from 0.3 to 0.95. Interpreting this reasonably accurately<br />

as being "charge purity" for the firing engine situation, it is clear that at light loads <strong>and</strong> low<br />

engine rotational speeds there will be a throttle position where the considerable mass <strong>of</strong> exhaust<br />

gas present will not permit ignition <strong>of</strong> the gasoline vapor-air mixture. When the spark<br />

occurs, the mass <strong>of</strong> vapor <strong>and</strong> air ignited in the vicinity <strong>of</strong> the spark is too small to provide an<br />

adequate release <strong>of</strong> heat to raise the surrounding layer <strong>of</strong> unburned mixture to the auto-ignition<br />

temperature. Consequently, the flame does not develop <strong>and</strong> combustion does not take<br />

place. The effect is somewhat similar to the lean burning misfire limit discussed above.<br />

During the next scavenging process the scavenging efficiency is raised as the "exhaust<br />

residual" during that process is composed partly <strong>of</strong> the unburned mixture from the misfire<br />

stroke <strong>and</strong> partly <strong>of</strong> exhaust gas from the stroke preceding that one. Should the new SE value<br />

prove to be over the threshold condition for flammability, then combustion does takes place.<br />

This skip firing behavior is called "four-stroking." Should it take a further scavenge process<br />

for the SE level to rise sufficiently for ignition to occur, then that would be "six-stroking,"<br />

<strong>and</strong> so on. Of course, the scavenging processes during this intermittent firing behavior eject<br />

considerable quantities <strong>of</strong> unburned fuel <strong>and</strong> air into the exhaust duct, to the very considerable<br />

detriment <strong>of</strong> the specific fuel consumption <strong>of</strong> the engine <strong>and</strong> its emission <strong>of</strong> unburned<br />

hydrocarbons.<br />

Active radical combustion<br />

It was shown by Onishi [4.33] that it is possible under certain conditions to ignite, <strong>and</strong><br />

ignite with great success, an air-fuel mixture in high concentrations <strong>of</strong> residual exhaust gas,<br />

i.e., at low SE values. This was confirmed by Ishibashi [4.34] <strong>and</strong> the engine conditions<br />

required are to raise the trapping pressure <strong>and</strong> temperature so that the exhaust residual remains<br />

sufficiently hot <strong>and</strong> active to provide an ignition source for the air-fuel mixture distributed<br />

through it. Hence the term "active radical," or AR, combustion. The ensuing combustion<br />

process is very stable, very efficient, <strong>and</strong> eliminates both the "four-stroking" skip firing regime<br />

<strong>and</strong> the high exhaust emissions <strong>of</strong> hydrocarbons that accompany it, as described above.<br />

It is certainly a design option open for the development <strong>of</strong> the simple carburetted engine <strong>and</strong><br />

one which has not been sufficiently exploited. There is some evidence that several motorcycle<br />

engines <strong>of</strong> the 1930s had low speed <strong>and</strong> low load combustion processes which behaved<br />

in this manner.<br />

The effect must not be confused with detonation, as discussed in the next section.<br />

4.1.4 Detonation or abnormal combustion<br />

Detonation occurs in the combustion process when the advancing flame front, which is<br />

pressurizing <strong>and</strong> heating the unburned mixture ahead <strong>of</strong> it, does so at such a rate that the<br />

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