3. The pressure, velocity and density perturbations for a one-dimensional acoustic wave are respectively given by p' = peik(x-ct), u' = ûeik(x-ct) and p = peik(x-ct). (a) Find the corresponding solutions for the zonal wind and density perturbations by relating û, p to p. These are known as polarization relations. may utilize the linearized equations of motion for u' and p' but you will have to linearize the nonlinear continuity to obtain an equation for p'. Note that " equation û. rho and û represent complex amplitudes, not unit vectors!]

Applications and Investigations in Earth Science (9th Edition)
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ISBN:9780134746241
Author:Edward J. Tarbuck, Frederick K. Lutgens, Dennis G. Tasa
Publisher:Edward J. Tarbuck, Frederick K. Lutgens, Dennis G. Tasa
Chapter1: The Study Of Minerals
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Just do part -A 

3. The pressure, velocity and density perturbations for a one-dimensional acoustic wave
are respectively given by p' = peik(x-ct), u' = ûeik(x-ct) and p′ = peik(x-ct).
p'
(a) Find the corresponding solutions for the zonal wind and density perturbations
by relating û, ô to p. These are known as polarization relations.
may utilize the linearized equations of motion for u' and p'
but you will have to linearize the nonlinear continuity
to obtain an equation for p'. Note that
equation
û, rho and p represent complex amplitudes, not unit vectors!]
(b) In general, the complex amplitude ô can be written as p = |p|eis where |p|
is the (real) amplitude and 6 is the (real) phase. Express the amplitude and
phase for u' and p' in terms of the amplitude and phase of p'. For the fixed
time t=0 sketch the variation of p', u', p' as a function of x for one wavelength.
"
Transcribed Image Text:3. The pressure, velocity and density perturbations for a one-dimensional acoustic wave are respectively given by p' = peik(x-ct), u' = ûeik(x-ct) and p′ = peik(x-ct). p' (a) Find the corresponding solutions for the zonal wind and density perturbations by relating û, ô to p. These are known as polarization relations. may utilize the linearized equations of motion for u' and p' but you will have to linearize the nonlinear continuity to obtain an equation for p'. Note that equation û, rho and p represent complex amplitudes, not unit vectors!] (b) In general, the complex amplitude ô can be written as p = |p|eis where |p| is the (real) amplitude and 6 is the (real) phase. Express the amplitude and phase for u' and p' in terms of the amplitude and phase of p'. For the fixed time t=0 sketch the variation of p', u', p' as a function of x for one wavelength. "
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