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Design and Simulation of Two Stroke Engines

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Chapter 5 - Computer Modeling <strong>of</strong> <strong>Engines</strong><br />

3 CYLINDER SUPERCHARGED ENGINE AT 3500 RPM<br />

EXHAUST<br />

\<br />

CHARGING<br />

EFFICIENCY<br />

CYLINDER<br />

0 100 200 300 400<br />

CRANKSHAFT ANGLE, deg. atdc on cylinder no.3<br />

Fig. 5.36(c) Open cycle pressures <strong>and</strong> charging for cylinder No. 3.<br />

charging efficiency curve commencing at 150° atdc. Further information on this topic is given<br />

in Fig. 5.37, for the purity <strong>and</strong> temperature in the scavenge ports at cylinder 1, an end cylinder.<br />

The blowback into the exit from the scavenge ports is considerable, with the purity dipping<br />

to 0.4 <strong>and</strong> the temperature rising to 600°C. It is almost bottom dead center before the<br />

situation has been recouped <strong>and</strong> the purity has risen again to unity. It is a much more extreme<br />

characteristic than that seen for a crankcase compression engine in Figs. 5.17 <strong>and</strong> 5.18. It also<br />

illustrates a common failing <strong>of</strong> supercharged designs, in that they are rarely endowed with<br />

adequate blowdown characteristics, for the cylinder backflow into the scavenge ports backs<br />

up the compressor, increasing the pumping losses significantly. <strong>Design</strong>ers <strong>of</strong> such engines<br />

should re-examine Figs. 3.40 <strong>and</strong> 3.41, for it is possible you may have initially considered the<br />

exhaust port width shown there as excessive. In the light <strong>of</strong> the evidence given here, you may<br />

wish to reconsider that opinion.<br />

The exhaust tuning <strong>of</strong> a three-cylinder engine<br />

The pressure characteristics within the exhaust pipe at the exhaust port are also shown in<br />

Figs. 5.36(a)-(c) for each <strong>of</strong> the three cylinders. Just prior to the closing <strong>of</strong> the exhaust port,<br />

there is a "plugging" pulse reminiscent <strong>of</strong> that seen for the racing engine in Fig. 5.34. While<br />

this engine does not have a tuned expansion chamber, the effect <strong>of</strong> employing the compact<br />

manifold is almost the same. The "plugging" pulse effect in this case is caused by another<br />

cylinder blowing down into the manifold. In the case <strong>of</strong> Fig. 5.36(a) for cylinder 1, the "plugging"<br />

pulse emanates from the opening <strong>of</strong> the exhaust port <strong>of</strong> cylinder 3. In Fig. 5.32(b) it is<br />

from cylinder 1; in Fig. 5.32(c) it is from cylinder 2. This information is gleaned from the<br />

firing order being 1-3-2. The effect is to hold the charging efficiency at its plateau level, in<br />

this case about 0.61. This behavior in the multi-cylinder engine is known as "cross-charging."<br />

405

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