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Troels Dyhr Pedersen.indd - Solid Mechanics

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Page 18 of 21<br />

diesel type chamber<br />

3 ATDC<br />

1 BTDC<br />

3 BTDC<br />

1000 3000 5000 f (Hz) 7000 9000<br />

Figure 21: Frequency distribution with the diesel bowl chamber piston<br />

The common feature of all the FFT analysis result is that the largest contribution to the total SPL is found in the<br />

lower part of the frequency band from 1-3 kHz. These frequencies cannot exist inside the cylinder, since the<br />

lowest resonance frequency is 5-6 kHz in all cases except for the ring shaped geometry, which has its primary<br />

resonance frequency at 4 kHz. The 4 kHz frequency is clearly present in the analysis for this piston crown (fig.<br />

16).<br />

Engine block resonance will however occur as a result of higher frequencies being transmitted through the<br />

structure. The connection between structure born noise and emitted noise was investigated by Andreae et al<br />

[10]. It was found that the general source of noise was not that which was directly transmitted, but that of<br />

engine structure resonance being exited by the transmitted noise.<br />

A great reduction in the noise level was achieved by moving the chambers away from the cylinder walls and<br />

into the piston. The total surface area and therefore heat transfer was however increased. The crevice volume<br />

with this and the following pistons was very large since it was not possible to fit piston rings. This resulted in a<br />

reduction of combustion efficiency. In terms of noise reduction the performance was similar. The crevice<br />

volume was however unchanged, so the combustion efficiency was still reduced<br />

Frequency response<br />

The frequency response of the engine is here defined by the ratio of the sound pressure measured outside the<br />

engine to the sound pressure generated in the cylinder. The response is calculated for the range of frequencies in<br />

the FFT. A short term average of 5 ms following the peak heat release was used to allow all established modes<br />

of vibration to be included.<br />

The response is converted to dB. Since -100 dB corresponds to an attenuation of 100,000, a SP of 100 kPa in<br />

the cylinder will result in a SP of 1 Pa outside the engine.<br />

Figure 22 is an example of the frequency response of the flat chamber. The response of the other piston crowns<br />

was found to follow this pattern. The response of the flat chamber was selected because it produces a wide<br />

range of frequencies in the cylinder and thus provides a good signal-to-noise ratio for the response curve.<br />

Sound pressure (Pa)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0

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