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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 />

A<br />

T<br />

T<br />

E<br />

N<br />

U<br />

A<br />

T<br />

I<br />

0<br />

N<br />

50<br />

40<br />

30"<br />

20<br />

dB<br />

10<br />

1275 Hz<br />

0 T i i r -T-1—I—I—\—l—I 'I' I—t—i—i—i—i i i—i—i—r<br />

1000 2000<br />

FREQUENCY, Hz<br />

BOX A BOXC<br />

ONE OFF 5<br />

08 HOLE<br />

16 OFF<br />

0 2.6 HOLES<br />

ABSORPTION<br />

SILENCER<br />

BOX A BOX B BOX C<br />

INPUT DATA INPUT DATA INPUT DATA<br />

LB= 150<br />

LB= 50<br />

DSB= 80<br />

DSB= 80<br />

DS3= 16<br />

DS3= 16<br />

TH= 1.5<br />

TH= 1.5<br />

NH= 1<br />

NH= 16<br />

D5H= 6<br />

D5H= 2.6<br />

T2C= 400<br />

T2C= 400<br />

r~| 1 I I 1—1 1 1—T"<br />

3000 4000<br />

Fig. 8.28 Silencer design for a small motorcycle engine using Progs. 8.1 <strong>and</strong> 8.2.<br />

The box A, a side-resonant silencer, has a single 8-mm-diameter hole in the 16 mm pipe<br />

with a 1.5-mm-thick wall. The exhaust temperature is assumed to be 400°C. Note that, if the<br />

real box has sloping walls as in the sketch, then the computed box volume may not ultimately<br />

agree with the actual box volume, in which case a modified length, Lb, should be inserted as<br />

data so that the calculation operates with a realistic box volume. You will underst<strong>and</strong> the<br />

importance <strong>of</strong> that statement more fully if the relevant acoustic theory is re-examined in Sec.<br />

8.5.2 <strong>and</strong> Eqs. 8.5.6-8.5.16. That comment aside, the computed acoustic transmission loss is<br />

seen to peak at 475 Hz, which is sufficiently close to the target frequency <strong>of</strong> 500 Hz for<br />

maximum suppression.<br />

582

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