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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 />

in the designed direction <strong>of</strong> the port. A later research paper by Smyth [3.17] shows this to be<br />

inaccurate, particularly for the main transfer ports in a loop-scavenged design, <strong>and</strong> there is<br />

further discussion <strong>of</strong> that in Sec. 3.5.4.<br />

Examples <strong>of</strong> the use <strong>of</strong> the calculation are given by Sweeney [3.23] <strong>and</strong> a precis <strong>of</strong> the<br />

findings is shown here in Figs. 3.21-30. The examples selected as illustrations are modified<br />

Yamaha cylinders, Nos. 14 <strong>and</strong> 12, the best <strong>and</strong> the worst <strong>of</strong> that group whose performance<br />

characteristics <strong>and</strong> scavenging behavior has already been discussed in Sec. 3.2.4. The computation<br />

simulates the flow conditions <strong>of</strong> these cylinders on the QUB single-cycle test apparatus<br />

so that direct comparison can be made with experimental results.<br />

(a) (b) (c) (d)<br />

Fig. 3.22 Yamaha cylinder No. 14 charge purity plots at 29° BBDC.<br />

(a) (b) (c) (d)<br />

Fig. 3.23 Yamaha cylinder No. 14 charge purity plots at 9° BBDC.<br />

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