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Design and Simulation of Two Stroke Engines

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<strong>Design</strong> <strong>and</strong> <strong>Simulation</strong> <strong>of</strong><strong>Two</strong>~<strong>Stroke</strong> <strong>Engines</strong><br />

tant to emphasize that slowing down the exit rate <strong>of</strong> exhaust gas flow during the blowdown<br />

phase inevitably leads to longer port timing durations <strong>and</strong> some reduction <strong>of</strong> trapping efficiency.<br />

This can be alleviated to some extent by making the exhaust port wider without unduly<br />

increasing the total timing duration, as the shallower area-time pr<strong>of</strong>ile necessary for<br />

noise reduction also permits a wider port without endangering the mechanical trapping <strong>of</strong> the<br />

piston ring by the timing edge.<br />

Even with a suitably pr<strong>of</strong>iled exhaust port timing edge, the pressure-time rise characteristics<br />

<strong>of</strong> an exhaust pulse in a two-stroke power unit is much faster than that in a four-stroke<br />

cycle engine where a poppet valve is employed to release exhaust gas from the cylinder. As<br />

already remarked, the noise spectrum from a rapidly rising exhaust pressure wave is "rich" in<br />

high-frequency content, irritating to the human ear.<br />

In Fig. 8.25 it can be seen that the shaping <strong>of</strong> the exhaust port can be conducted in the<br />

same fashion as for the bottom <strong>of</strong> the inlet port. However, Johnston [8.14] shows more extreme<br />

pr<strong>of</strong>iles than the simple radiusing <strong>and</strong> proposed the "Q" port shape shown on the same<br />

figure, with a view to enhancing the effects already discussed.<br />

<strong>Simulation</strong> <strong>of</strong> the effect by engine modeling<br />

In the input data to the chainsaw engine simulation, both the exhaust <strong>and</strong> intake ports<br />

have a maximum width <strong>of</strong> 28 mm. The simulation result, described above as F, is compared<br />

with heavily radiused intake <strong>and</strong> exhaust ports, labeled as R. The original top <strong>and</strong> bottom<br />

radii for the intake <strong>and</strong> exhaust ports is 2 <strong>and</strong> 3 mm, respectively. For the simulation <strong>of</strong> R, this<br />

radius is increased to 10 mm in both cases. However, this reduces the port area <strong>and</strong> so it is<br />

necessary to open the exhaust port 1 ° earlier, at 107° atdc, <strong>and</strong> to open the inlet port 3° earlier,<br />

at 78° btdc, so as to provide for the same delivery ratio to pass through the engine. The result<br />

<strong>of</strong> the simulation <strong>of</strong> design R is shown in Table 8.5, where it is compared with design F.<br />

The reduction <strong>of</strong> intake <strong>and</strong> exhaust noise as forecast by the theory is achieved, even<br />

though the modification <strong>of</strong> changing the port radii from 2 or 3 mm to 10 mm is a relatively<br />

modest change, by comparison with the "Q port" shown in Fig. 8.25. The equality <strong>of</strong> delivery<br />

i<br />

NORMAL<br />

§1<br />

l-l-<br />

E5 RADIUSED<br />

STEEP FRONTED<br />

PULSE<br />

t<br />

SHALLOWER<br />

PROFILE<br />

Fig. 8.25 Exhaust port pr<strong>of</strong>iling to reduce noise.<br />

578

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