The significant noise sources originate in the fan or compressor, the
turbine, and the exhaust jet or jets. The generation of the noise from
these components increases with greater relative airflow velocity.
Exhuast jet noise varies by a larger factor than that of the compressor or
turbine, so a reduction of exhaust velocity has a stronger influence than
equivalent reductions in the others.
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Jet exhaust noise is caused by the violent turbulent mixing of the exhaust
gases with the atmosphere and is influenced by the shearing action
caused by the relative speeds between the exhaust jet and the atmosphere.
Turbulence created near the exhaust exit causes a high frequency noise
(small eddies) and further downstream of the exhaust, turbulence causes
low frequency noise (large eddies).
In addition, a shock wave is formed
when the exhaust velocity exceeds the speed of sound. A reduction in
noise level can be accomplished when the mixing rate is accelerated or the
exhaust velocity relative to the atmosphere is reduced. This can
be achieved by changing the pattern of the exhaust jet as shown.
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Compressor and turbine noise results from the interaction of pressure
fields and turbulence for rotating blades and stationary vanes. Within
the jet engine, the exhaust jet noise is of such high level that the
turbine and compressor noise is insignificant during most operating
conditions. However, low landing-approach thrusts cause a drop in exhaust
jet noise and an increase in low pressure compressor and turbine noise due
to greater internal power handling. The introduction of a single stage
low pressure compressor significantly reduces the compressor noise because
the overall turbulence and interaction levels are diminished. Also, the
combustion chamber is another source of noise within the engine. However,
because it is 'buried' within the engine's core, it does not have a
predominant contribution.
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Mentioned earlier, the exhaust jet is the major source of jet engine
noise. This can be suppressed by inducing a rapid or shorter mixing
region. Where this reduces the low frequency level, it may increase the
high frequency noises, which are quickly absorbed by the atmosphere. Thus
the noise that does reach the listener is outside the audible range. This
is achieved by increasing the contact area between the exhaust gas stream
and the atmosphere by using a nozzle incorporating a corrugated or
lobe-type noise suppressor.
Deep corrugations, lobes, or multi-lobes give the largest reduction in
noise level, but performance penalties limit the depth or number of
corrugations or lobes. The same overall area as the basic nozzle must be
kept, so when using this method, the final diameter of the supressor may
have to be increased causing excessive drag and weight results.
Again, the noise reduction principle is to minimize the exhaust jet
velocity while still mainting performance objectives. The most successful
method used is to mix the hot and cold exhaust streams within the engine
and expel the lower exhaust gases through a single nozzle.
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Research has produced a good understanding of noise generation and
comprehensive noise design rules exist. These are founded on the need to
minimize turbulence levels, reduce the strength of interactions between
rotating blades and stationary vanes, and optimizing the use of
acoustically absorbent linings.
Noise absorbing 'lining' material converts acoustic
energy into heat. These linings normally consist of a porous skin
supported by a honeycomb backing and provide a seperation between the
facesheet and the engine duct. For optimum suppression, the acoustic
properties of the skin and the liner are carefully matched to the noise
character.
A disadvantage of these lining materials is the slight increase in weight
and surface drag, resulting in an increase in overall fuel consumption.
However, they do provide a very powerful noise suppression technique.
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