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Troels Dyhr Pedersen.indd - Solid Mechanics

Troels Dyhr Pedersen.indd - Solid Mechanics

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The frequency content of the acoustic noise generated in the cylinder is important since these frequencies are<br />

transmitted directly to the surroundings but with different efficiency due to the frequency response of the<br />

engine. The nature of in-cylinder oscillations in cylindrical chambers were investigated by [6], [7] and [8].<br />

These studies showed that the resonance frequencies in a cylindrical combustion chamber follow acoustic<br />

theory for closed cylindrical chambers.<br />

The lowest resonance mode in a cylindrical chamber is a transverse wave with a single node through the center<br />

of the cylinder as shown to the left in figure 1. This mode usually has the highest amplitude. In the figure, dark<br />

represents high and low pressure zones and bright shows the node between them. The pressure zones shift from<br />

high to low and back again at the given frequencies. The frequency of the modes in figure 1 are calculated at a<br />

temperature of 1900 K in a chamber with a diameter of 85 mm.<br />

Figure 1: Illustration of resonance modes in a cylindrical chamber. From the left, the modes and corresponding<br />

frequencies are: (1, 0): 5.9 kHz; (2, 0): 9.7 kHz, (0, 1): 12.2 kHz and (3, 0) 15.5 kHz<br />

The index (a, b) refers to circumferential and radial modes of vibration. There is also a third mode which is the<br />

axial modes, but due to the limited distance between piston and cylinder head the axial modes have very high<br />

frequencies and are rarely exited at magnitudes of importance. In experiments the first circumferential mode (1,<br />

0) is most often dominating, while the first radial mode (0, 1) and the second circumferential mode (2, 0) are<br />

present at lower amplitudes. Higher modes can be present, but their amplitudes are generally much lower than<br />

the first circumferential mode.<br />

When looking at the chamber geometries which are presented on the next pages, the theory for cylindrical<br />

cavities does no longer support accurate calculations of the frequencies. In general however, similar patterns<br />

will be established in the chamber while the differences in piston geometry will alter the frequencies and<br />

possibly reduce the amplitudes.<br />

EXPERIMENTAL SETUP<br />

PISTON CROWNS<br />

Being the focus of this study, these piston crowns are presented first. Seven different types were designed for<br />

the study. All piston crowns were designed to a compression ratio of 10. In all cases, except for the flat piston<br />

crown, the distance from piston top to cylinder head was 1 mm, which was the minimum requirement for<br />

avoiding valve contact.<br />

The purpose was first of all to test different geometries that could possibly reduce the interaction between<br />

pressure and reaction rate, in order to avoid the larger pressure oscillations found in the typical cylindrical<br />

chamber.<br />

The cylindrical chamber is formed by a flat piston crown (fig. 2) which has a compression height (distance to<br />

the cylinder head) of eight millimeters. The acoustic behavior of the flat piston is relevant in SI type combustion<br />

Page 3 of 21

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