15.02.2013 Views

Design and Simulation of Two Stroke Engines

Design and Simulation of Two Stroke Engines

Design and Simulation of Two Stroke Engines

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

LU<br />

hoQ<br />

ft<br />

CO<br />

1.0 -i<br />

0.8<br />

g0.6<br />

LU<br />

o<br />

LL 0.4<br />

LU<br />

0.2<br />

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

YAMAHA CYLINDER 12<br />

1<br />

SCAVENGE RATIO, SRv<br />

SEv THEORY<br />

TEv THEORY<br />

SEv EXP<br />

TEv EXP<br />

Fig. 3.30 Comparison <strong>of</strong> experiment <strong>and</strong> CFD computation.<br />

In terms <strong>of</strong> insight, Figs. 3.21-3.24 <strong>and</strong> 3.25-3.28 show the in-cylinder charge purity<br />

contours for cylinders 14 <strong>and</strong> 12, respectively. In each figure are four separate cylinder sections<br />

culled from the cells in the calculation. The cylinder section (a) is one along the plane <strong>of</strong><br />

symmetry with the exhaust port to the right. The cylinder section (b) is at right angles to<br />

section (a). The cylinder section (c) is on the surface <strong>of</strong> the piston with the exhaust port to the<br />

right. The cylinder section (d) is above section (c) <strong>and</strong> halfway between the piston crown <strong>and</strong><br />

the cylinder head. In Fig. 3.21(a) <strong>and</strong> Fig. 3.25(a) it can be seen from the flow at 39° bbdc that<br />

the short-circuiting flow is more fully developed in cylinder 12 than in cylinder 14. The SEV<br />

level at the exhaust port for cylinder 14 is 0.01 whereas it is between 0.1 <strong>and</strong> 0.2 for cylinder<br />

12. This situation gets worse by 29° bbdc, when the SEV value for cylinder 14 is no worse than<br />

0.1, while for cylinder 12 it is between 0.1 <strong>and</strong> 0.4. This flow characteristic persists at 9°<br />

bbdc, where the SEV value for cylinder 14 is between 0.1 <strong>and</strong> 0.2 <strong>and</strong> the equivalent value for<br />

cylinder 12 is as high as 0.6. By 29° abdc, the situation has stabilized with both cylinders<br />

having SEV values at the exhaust port <strong>of</strong> about 0.6. For cylinder 12, the damage has already<br />

been done to its scavenging efficiency before the bdc piston position, with the higher rate <strong>of</strong><br />

fresh charge flow to exhaust by short-circuiting. This ties in precisely with the views <strong>of</strong> Sher<br />

[3.24] <strong>and</strong> also with my simple scavenge model in Sec. 3.3.2, regarding the ne-SRv pr<strong>of</strong>ile at<br />

the exhaust port, as shown in Fig. 3.18.<br />

Typical <strong>of</strong> a good scavenging cylinder such as cylinder 14 by comparison with bad scavenging<br />

as in cylinder 12 is the sharp boundary between the "up" <strong>and</strong> the "down" parts <strong>of</strong> the<br />

looping flow. This is easily seen in Figs. 3.23 <strong>and</strong> 3.27. It is a recurring feature <strong>of</strong> all loopscavenged<br />

cylinders with good scavenging behavior, <strong>and</strong> this has been observed many times<br />

by the research team at QUB.<br />

249

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!