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Design and Simulation of Two Stroke Engines

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Q<br />

Chapter 2 - Gas Flow through <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

gas at Te <strong>and</strong> p^V-^<br />

(a) compression pressure wave<br />

(b) expansion pressure wave<br />

Fig. 2.1 Pressure wave nomenclature.<br />

oce. It is also moving gas particles at a gas particle velocity <strong>of</strong> ce <strong>and</strong> in the same direction as<br />

the wave is being propagated. At a point on the expansion wave in the pipe the pressure is pj,<br />

where p; < po, <strong>and</strong> it is being propagated at a velocity, (Xj. It is also moving gas particles<br />

at a gas particle velocity <strong>of</strong> q, but in the opposite direction to that which the wave is<br />

being propagated.<br />

At this point you can draw on your personal experience <strong>of</strong> sound waves to help underst<strong>and</strong><br />

the physical nature <strong>of</strong> the statements made in the preceding paragraph. Imagine st<strong>and</strong>ing<br />

several meters away from another person, Fred. Fred produces a sharp exhalation <strong>of</strong><br />

breath, for example, he says "boo" somewhat loudly. He does this by raising his lung pressure<br />

above the atmospheric pressure due to a muscular reduction <strong>of</strong> his lung volume. The compression<br />

pressure wave produced, albeit <strong>of</strong> small amplitude, leaves his mouth <strong>and</strong> is propagated<br />

at the local acoustic velocity, or speed <strong>of</strong> sound, to your ear. The speed <strong>of</strong> sound involved<br />

is on the order <strong>of</strong> 350 m/s. The gas particles involved with the "boo" leaving Fred's<br />

mouth have a much lower velocity, probably on the order <strong>of</strong> 1 m/s. However, that gas particle<br />

velocity is in the same direction as the propagation <strong>of</strong> the compression pressure wave, i.e.,<br />

toward your ear. Contrast this simple experiment with a second test. Imagine that Fred now<br />

produces a sharp inhalation <strong>of</strong> breath. This he accomplishes by exp<strong>and</strong>ing his lung volume so<br />

that his lung pressure falls sharply below the atmospheric pressure. The resulting "u....uh"<br />

you hear is caused by the expansion pressure wave leaving Fred's mouth <strong>and</strong> propagating<br />

toward your ear at the local acoustic velocity. In short, the direction <strong>of</strong> propagation is the<br />

same as before with the compression wave "boo," <strong>and</strong> the propagation velocity is, to all<br />

intents <strong>and</strong> purposes, identical. However, as the gas particles manifestly entered Fred's mouth<br />

with the creation <strong>of</strong> this expansion wave, the gas particle velocity is clearly opposite to the<br />

direction <strong>of</strong> the expansion wave propagation.<br />

53<br />

D

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