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Design and Simulation of Two Stroke Engines

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Chapter 3 - Scavenging the <strong>Two</strong>-<strong>Stroke</strong> Engine<br />

relevant criteria for dynamic similarity. It is a dynamic experiment, for the piston moves <strong>and</strong><br />

provides the realistic attachment behavior <strong>of</strong> scavenge flow as it would occur in the actual<br />

process in the firing engine. Sweeney [3.20, 3.23] demonstrates the repeatability <strong>of</strong> the test<br />

method <strong>and</strong> <strong>of</strong> its excellent correlation with experiments conducted under firing conditions.<br />

Some <strong>of</strong> those results are worth repeating here, for that point cannot be emphasized too strongly.<br />

The experimental performance characteristics, conducted at full throttle for a series <strong>of</strong><br />

modified Yamaha DT 250 engine cylinders, are shown in Fig. 3.7. Each cylinder has identical<br />

engine geometry so that the only modifications made were to the directioning <strong>of</strong> the transfer<br />

ports <strong>and</strong> the shape <strong>of</strong> the transfer duct. Neither port timings nor port areas were affected so<br />

that each cylinder had almost identical SR characteristics at any given rotational speed. Thus,<br />

the only factor influencing engine performance was the scavenge process. That this is significant<br />

is clearly evident from that figure, as the bmep <strong>and</strong> bsfc behavior is affected by as much<br />

as 15%. When these same cylinders were tested on the single-cycle gas scavenging rig, the<br />

SEV-SRV characteristics were found to be as shown in Fig. 3.8. The figure needs closer examination,<br />

so a magnified region centered on a SRV value <strong>of</strong> 0.9 is shown in Fig. 3.9. Here, it can<br />

be observed that the ranking order <strong>of</strong> those same cylinders is exactly as in Fig. 3.7, <strong>and</strong> so too<br />

is their relative positions. In other words, Cylinders 14 <strong>and</strong> 15 are the best <strong>and</strong> almost as<br />

effective as each other, so too are cylinders 9 <strong>and</strong> 7 but at a lower level <strong>of</strong> scavenging efficiency<br />

<strong>and</strong> power. The worst cylinder <strong>of</strong> the group is cylinder 12 on all counts. The "double<br />

indemnity" nature <strong>of</strong> a loss <strong>of</strong> 8% SEV at a SRV level <strong>of</strong> 0.9, or a TEV drop <strong>of</strong> 9%, is translated<br />

into the bmep <strong>and</strong> bsfc shifts already detailed above at 15%.<br />

A sustained research <strong>and</strong> development effort has taken place at QUB in the experimental<br />

<strong>and</strong> theoretical aspects <strong>of</strong> scavenging flow. For the serious student <strong>of</strong> the subject, the papers<br />

published from QUB form a series, each using information <strong>and</strong> thought processes from the<br />

preceding publication. That reading list, in consecutive order, is [3.6], [1.23], [3.13], [3.20],<br />

[1.10], [3.23], [1.11], <strong>and</strong> [3.17].<br />

3.2.4 Comparison <strong>of</strong> loop, cross <strong>and</strong> uniflow scavenging<br />

The QUB single-cycle gas scavenge experiment permits the accurate <strong>and</strong> relevant comparison<br />

<strong>of</strong> SEV-SRV <strong>and</strong> TEV-SRV characteristics <strong>of</strong> different types <strong>of</strong> scavenging. From some<br />

<strong>of</strong> those previous papers, <strong>and</strong> from other experimental work at QUB hitherto unpublished,<br />

test results for uniflow-, loop- <strong>and</strong> cross-scavenged engine cylinders are presented to illustrate<br />

the several points being made. At this stage the most important issue is the use <strong>of</strong> the<br />

experimental apparatus to compare the various methods <strong>of</strong> scavenging, in order to derive<br />

some fundamental underst<strong>and</strong>ing <strong>of</strong> the effectiveness <strong>of</strong> the scavenging process conducted by<br />

these several methodologies. In Sec. 3.3 the information gained will be used to determine the<br />

theoretical relevance <strong>of</strong> this experimental data in the formulation <strong>of</strong> a model <strong>of</strong> scavenging to<br />

be incorporated within a complete theoretical model <strong>of</strong> the firing engine.<br />

Figs. 3.10-3.13 give the scavenging <strong>and</strong> trapping characteristics for eight engine cylinders,<br />

as measured on the single-cycle gas scavenging rig. It will be observed that the test<br />

results fall between the perfect displacement line <strong>and</strong> perfect mixing line from the theories <strong>of</strong><br />

Hopkinson [3.1]. By contrast, as will be discussed in Sec. 3.3, some <strong>of</strong> the data presented by<br />

others [3.3, 3.4] lie below the perfect mixing line.<br />

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