

4 Application of
Models
The criteria for choosing a
particular model are determined from the dual considerations of the potential
application and the desired accuracy:
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Two of the available models,
the two-dimensional viscous incompressible flow model and the one-dimensional
viscous compressible flow model, are not considered to be well suited
to the modelling of fluid transmission lines. The two-dimensional incompressible
flow model is accurate in predicting instantaneous velocity profiles,
and the series impedance is readily obtained from it. However, it is necessary
to introduce further assumptions concerning the nature of propagation to
obtain approximate expressions for the characteristic impedance and propagation
operator. As the compressibility effects do not complicate the solution,
the two-dimensional viscous compressible model should be used in
preference.
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The one-dimensional viscous
compressible flow model is based upon the assumption that disturbances
propagate as plane waves along the tube. Because it ignores the effects
of velocity profile in the line, the actual losses occurring due to viscosity
are grossly underestimated. For most practical applications this model
and the one-dimensional inviscid compressible model could be considered
to be equivalent.
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The 'exact' first-order
model contains more detail than is necessary to cover the majority of engineering
applications. Gerlach and Parker [45]
have shown that the radial propagation modes are damped out within a couple
of pipe radii of the end of the transmission line. Gerlach [61]
and Urata [46] have demonstrated
that the solution obtained using this model is identical to the solution
to the two-dimensional viscous compressible model, assuming that
plane wave attenuation effects and the radial pressure distribution are
negligible.
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In their review of fluid transmission
line models Goodson and Leonard [62]
have shown that the choice between the two-dimensional viscous compressible
model and the one-dimensional inviscid compressible model is determined
by the relative size of the viscous losses occurring in the line compared
with the resistive losses occurring at the load impedance. When considering
the frequency response of a blocked line, they recommended that the viscous
model should be used in all cases except where the driving frequency is
well below the fundamental frequency of the line. The use of the two-dimensional
thermal viscous compressible model is determined by the ratio of specific
heats and the Prandtl number of the fluid. Further study reported in [55]
and [10] carried out using
alternating flow test rig confirmed that two-dimensional viscous compressible
is most suitable for modelling of long transmission lines When the
Prandtl number is small and the ratio of specific heats is greater than
unity, as is the case for most gases, the thermal effects become significant
and this model should be used. For liquids, the ratio of specific heats
is generally close to one and the thermal losses are negligible.
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The one-dimensional linear
resistance compressible model can be applied in many cases but it is
difficult to give general considerations on its use, as the limits of application
depend on the chosen form of resistance coefficient. This in turn limits
the frequency response over which the model can accurately be applied.

