3. The pressure, velocity and density perturbations for a one-dimensional acoustic wave are respectively given by p' = pei 。ik(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, ô to ô. These are known as polarization relations. [Hint: you may utilize the linearized equations of motion for u' and p' [in the notes or HH5 (5.20) and (5.21)], but you will have to linearize the nonlinear continuity equation [in the notes or HH5 (5.15)] to obtain an equation for p'. Note that û, rho and ô 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. [HH 5.4]
3. The pressure, velocity and density perturbations for a one-dimensional acoustic wave are respectively given by p' = pei 。ik(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, ô to ô. These are known as polarization relations. [Hint: you may utilize the linearized equations of motion for u' and p' [in the notes or HH5 (5.20) and (5.21)], but you will have to linearize the nonlinear continuity equation [in the notes or HH5 (5.15)] to obtain an equation for p'. Note that û, rho and ô 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. [HH 5.4]
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There is sketch in part B of this section please try to sketch the diagram. Show step by step how you reach for each section answer and also use letter used in this question it would be great
![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, ô to p. These are known as polarization relations. [Hint: you
may utilize the linearized equations of motion for u' and p' [in the notes or
HH5 (5.20) and (5.21)], but you will have to linearize the nonlinear continuity
equation [in the notes or HH5 (5.15)] to obtain an equation for p'. Note that
û, rho and p represent complex amplitudes, not unit vectors!]
(b) In general, the complex amplitude ô can be written as p ples where p
is the (real) amplitude and d 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.
[HH 5.4]
=](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F8599088d-d6bb-412b-9dca-c57ae067f3ab%2F66f5ba8c-2879-4f7c-ac1b-48275316dea5%2Feju8t4c_processed.png&w=3840&q=75)
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).
=
(a) Find the corresponding solutions for the zonal wind and density perturbations
by relating û, ô to p. These are known as polarization relations. [Hint: you
may utilize the linearized equations of motion for u' and p' [in the notes or
HH5 (5.20) and (5.21)], but you will have to linearize the nonlinear continuity
equation [in the notes or HH5 (5.15)] to obtain an equation for p'. Note that
û, rho and p represent complex amplitudes, not unit vectors!]
(b) In general, the complex amplitude ô can be written as p ples where p
is the (real) amplitude and d 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.
[HH 5.4]
=
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