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Design and Simulation of Two Stroke Engines

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Chapter 8 - Reduction <strong>of</strong> Noise Emission from <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

splits the total box volume into two parts, labeled as Vi <strong>and</strong> V2, <strong>and</strong> the simulation models the<br />

entire system as two complete boxes separated by the filter element in precisely the same<br />

fashion that it does for the exhaust system. The geometry is detailed in Table. 8.1.<br />

Name<br />

S<br />

E<br />

F<br />

G<br />

df<br />

(mm)<br />

30<br />

30<br />

30<br />

30<br />

Table 8.1 Intake silencer geometry for the chainsaw<br />

d2<br />

(mm)<br />

22<br />

22<br />

22<br />

22<br />

dp<br />

(mm)<br />

22<br />

17<br />

15<br />

19<br />

LP<br />

(mm)<br />

50<br />

160<br />

125<br />

200<br />

V1<br />

(cm 3 )<br />

200<br />

200<br />

200<br />

200<br />

v2<br />

(cm 3 )<br />

100<br />

300<br />

300<br />

300<br />

fi<br />

(Hz)<br />

240<br />

88.9<br />

88.3<br />

80.1<br />

It will be seen that those characterized in Table 8.1 above as E, F, <strong>and</strong> G are the various<br />

alternatives as designed by the acoustic criteria, whereas that called S is the original "st<strong>and</strong>ard"<br />

system.<br />

The unsteady gas-dynamic simulation prepares an output file <strong>of</strong> the mass flow-time history<br />

at the intake from the atmosphere. For the four systems analyzed, this is shown in Fig.<br />

8.19 as the results <strong>of</strong> simulation at 9600 rpm, at a slightly different, i.e., leaner, air-to-fuel<br />

ratio than that employed for the more complete data map in Fig. 5.9. The theory <strong>of</strong> Sec. 8.4.1<br />

conducts a Fourier analysis <strong>of</strong> the data in Fig. 8.19 <strong>and</strong> produces the noise spectra shown in<br />

Fig. 8.20, at a distance, rm, <strong>of</strong> 1.0 m from the intake <strong>and</strong> exhaust exit points, at an orientation<br />

angle, 0, <strong>of</strong> zero. Not surprisingly, the more open silencer, S, has the greater mass flow fluctuations<br />

<strong>and</strong> has a higher noise spectra pr<strong>of</strong>ile than any <strong>of</strong> the more optimized silencers, E, F<br />

or G. They are all reasonably similar, but the silencer, F, has the smoothest mass flow-time<br />

history <strong>and</strong> comes out with the lowest peak noise level at 640 Hz, the fourth harmonic. Thus<br />

the design, F, one <strong>of</strong> those determined above by the acoustic criteria, emerges as being superior<br />

from a noise st<strong>and</strong>point to the st<strong>and</strong>ard silencer, S. The overall noise levels, the summations<br />

<strong>of</strong> these spectra, are given in Table 8.2.<br />

Name<br />

S<br />

E<br />

F<br />

G<br />

Table 8.2 Performance <strong>and</strong> intake silencing for the chainsaw<br />

Intake<br />

(dBlin)<br />

103.6<br />

92.2<br />

90.1<br />

93.8<br />

Intake<br />

(dBA)<br />

98.5<br />

87.2<br />

82.9<br />

89.5<br />

Exhaust<br />

(dBA)<br />

89.0<br />

88.8<br />

88.8<br />

88.8<br />

Total<br />

(dBA)<br />

99.0<br />

91.1<br />

89.8<br />

92.2<br />

bmep<br />

(bar)<br />

3.65<br />

3.82<br />

3.79<br />

3.79<br />

DR<br />

0.525<br />

0.546<br />

0.541<br />

0.550<br />

The intake geometry <strong>of</strong> F is overall quieter than E <strong>and</strong> G by 4 dB or more. That is very<br />

much quieter, for, recall from Eq. 8.1.6, two equal sound sources give an increase <strong>of</strong> approximately<br />

3 dB. The acoustic criteria gave no guidance on this matter. The st<strong>and</strong>ard silencer, S,<br />

is actually noisier than the exhaust system.<br />

571

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