Troels Dyhr Pedersen.indd - Solid Mechanics
Troels Dyhr Pedersen.indd - Solid Mechanics
Troels Dyhr Pedersen.indd - Solid Mechanics
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11.7 Theory of cylinder acoustics<br />
Cylinder pressure oscillations are initiated by the strong pressure gradients formed when<br />
the combustion proceeds unevenly in the chamber. The pressure gradient may be created<br />
by a confined explosion in the charge due to spatial variation in fuel or temperature<br />
distribution, or a developing detonation, which are discussed in the next chapter.<br />
Once a pressure difference is introduced, the pressure will drive the gas towards the low<br />
pressure area. The momentum of the gas means that the gas will continue into the low<br />
pressure region even after pressure equalization, thereby increasing the pressure to that of<br />
the former high pressure region. The pressure distribution is now reversed and the gas<br />
will be forced back to its origin. This behavior is known as resonance.<br />
Established resonance modes in the cylindrical geometry fall in to three categories:<br />
circumferential modes, radial modes and axial modes. These are explained in the<br />
following subsections. The modes may appear simultaneously by the principle of<br />
superposition as shown in table 5.<br />
11.7.1 Circumferential modes<br />
If the charge is pushed from one side of the cylinder wall it will oscillate across the<br />
chamber in a transverse motion. This situation is equivalent to pushing a glass of water,<br />
which forces the water into moving from side to side. The first mode has one node which<br />
runs through the diameter of the cylinder. All of the fluid moves from the low pressure to<br />
the high pressure zone across the chamber. This mode is therefore the most powerful in<br />
terms of momentum transport.<br />
The second mode has two nodes that are orthogonal and hence two high pressure zones<br />
that must be opposite. The gas does not move across the two symmetry lines. The gas<br />
movement takes places from the sides of the high pressure zones to the sides of the low<br />
pressure zones. In this case the gas movement is split into four directions. This means that<br />
less energy is transported across the chamber and hence less energy is transferred to the<br />
walls by momentum and heat transfer. So, despite being measurable in the chamber, this<br />
mode is less important in terms of energy losses and transmitted sound.<br />
11.7.2 Radial modes<br />
If the pressure rises in the center (or throughout the entire perimeter simultaneously) it<br />
will create a radial wave moving from the center towards the cylinder liner. This<br />
corresponds to the familiar rings that form when a drop of water hits the surface of a<br />
water pool. Like in a glass of water, the wave is reflected back towards the center.<br />
The first mode of vibration has a high and low pressure zone and a circular node. The<br />
higher nodes that may be formed have more pressure zones in the same ring pattern. As<br />
with the transverse waves, only the lowest mode carries enough momentum to be<br />
important.