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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 />

DELIVERY RATIO<br />

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CC END INLET DUCT X ^ ^ ^ ^<br />

AIR BOX END<br />

OF INLET DUCT CRANKCASE<br />

100<br />

1 • 1 •<br />

200 300<br />

CRANKSHAFT ANGLE, deg. atdc<br />

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Fig. 5.24 Pressure related to airflow in a chainsaw at 9600 rpm.<br />

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OF INTAKE<br />

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1 1 • 1 1-<br />

100 200 300<br />

CRANKSHAFT ANGLE, deg. atdc<br />

AIR BOX END<br />

OF INTAKE<br />

Fig. 5.25 Temperatures in the intake system <strong>of</strong> a chainsaw at 9600 rpm.<br />

The crankcase pressure has already dropped to 0.8 atm by the time the inlet port opens,<br />

sending a sharp, i.e., noisy, pulsation as an intake wave into the inlet duct, which peaks at<br />

about the tdc position. The ensuing crankcase pumping action raises its pressure to about 1.5<br />

atm, aided at that juncture by the higher pressure cylinder backflow into the scavenge ducts,<br />

as discussed above.<br />

The temperatures throughout the intake process are shown in Fig. 5.25 for the crankcase<br />

air <strong>and</strong> at both ends <strong>of</strong> the intake duct. Heat transfer in the crankcase <strong>and</strong> inlet tract is responsible<br />

for the dichotomy which exists. The air in the crankcase never drops below 60°C, whereas<br />

most <strong>of</strong> the air in the inlet duct oscillates around 40°C. During induction into the crankcase,<br />

391<br />

400

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