The “inversion theorem” for Fourier transforms states that

ϕ~(z)=-Φ~(k)eikzdkΦ~(k)=12π-ϕ~(z)e-kzdz

Short Answer

Expert verified

The expression forA~(k)is12π-f(z,0)+iωf(z,0)e-ikzdz

Step by step solution

01

Expression for the linear combination of sinusoidal wave:

Write the expression for the linear combination of a sinusoidal wave.

f~(z,t)=-A~(k)ei(kz-ωt)dk …… (1)

Here, kis the propagation vector and ωis the angular frequency.

02

Determine in A ̃(k) term of f(z,0) and f*(z,0).

Substitute t=0in equation (1).

f~(z,0)=-A~(k)ei(kz-ω(0))dk

=-A~(k)eikzdk

Write the conjugate of the above expression.

f~(z,0)=-A~(-k)e-ikzdkf~(z,0)=-A~(k)e-ikz(-dk)

It is known that,

f(z,0)=Re[f~(z,0)]

f(z,0)=12f~(z,0)+f~(z,0)* …… (2)

Substitute 12A~(k)eikzdkforf~(z,0)and12A~(-k)*eikzdkforf~(z,0)*in equation

(2).

f(z,0)=-12A~(k)+A~(-k)*eikzdk

Substitute f(z,0)=-12A~(k)+A~(-k)*eikzdkin equation (2).

12A~(k)+A~(-k)*=12π-f(z,0)e-ikzdz…… (3)

Solve the conjugate of f̃(z,0)

f~(z,t)=-A~(k)(-iω)ei(kz-ωt)dkf~(z,t)=-[-iωA~(k)]eikzdkf~(z,0)*=--iωA~(k)*e-ikzdkf~(z,0)*=-iωA~(k)*e-ikz(-dk)

On further solving, the above equation becomes,

f~(z,0)*=-iωA~(-k)*e-ikz(dk)f(z,0)=Re[f~(z,0)]

f(z,0)=12f~(z,0)+f~(z,0)* …… (4)

Substitute12-iωA~(k)eikzdkforf~(z,0)and12-iωA~(k)*eikzdkforf~(z,0)*for and for in equation (4).

f(z,0)=-12[-iωA~(k)+iωA~(-k)]eikzdkf(z,0)=-iω2A~(k)-A~(-k)*

The inversion theorem for Fourier transformation states that,

f(z,0)=12π-f(z,0)e-ikzdz

Equate both the values of f(z,0)

12A~(k)-A~(-k)*=12π-iωf(z,0)e-ikzdz …… (5)

Add equations (3) and (5).

12A~(k)+A~(-k)*+12A~(k)-A~(-k)*=12π-f(z,0)e-ikzdz+12π-iωf(z,0)e-ikzdz

role="math" localid="1657466135705" A~(k)=12π-f(z,0)+iωf(z,0)e-ikzdz

Therefore, the required expression isA~(k)=12π-f(z,0)+iωf(z,0)e-ikzdz

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Most popular questions from this chapter

Question: Obtain Eq. 9.20 directly from the wave equation by separation of variables.

A microwave antenna radiating at 10GHz is to be protected from the environment by a plastic shield of dielectric constant 2.5. What is the minimum thickness of this shielding that will allow perfect transmission (assuming normal incidence)? [Hint: Use Eq. 9. 199.]

A microwave antenna radiating at 10GHzis to be protected from the environment by a plastic shield of dielectric constant2.5. . What is the minimum thickness of this shielding that will allow perfect transmission (assuming normal incidence)? [Hint: Use Eq. 9.199.]

Question:Equation 9.36 describes the most general linearly polarized wave on a string. Linear (or "plane") polarization (so called because the displacement is parallel to a fixed vector n) results from the combination of horizontally and vertically polarized waves of the same phase (Eq. 9.39). If the two components are of equal amplitude, but out of phase by (say,δν=0,δh=90°,), the result is a circularly polarized wave. In that case:

(a) At a fixed point, show that the string moves in a circle about the axis. Does it go clockwise or counter clockwise, as you look down the axis toward the origin? How would you construct a wave circling the other way? (In optics, the clockwise case is called right circular polarization, and the counter clockwise, left circular polarization.)

(b) Sketch the string at time t =0.

(c) How would you shake the string in order to produce a circularly polarized wave?

Suppose you send an incident wave of specified shape, g1(z-v1t), down string number 1. It gives rise to a reflected wave, hR(z+v1t), and a transmitted wave, gT(z+v2t). By imposing the boundary conditions 9.26 and 9.27, find hRand gT.

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