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The "inversion theorem" for Fourier transforms states that

ฯ•(Z)=โˆซ-โˆžโˆžฯ•(k)eikzdkโ‡”ฯ•(k)=12ฯ€โˆซ-โˆžโˆžฯ•(z)e-ikzdz

Use this to determine A(k), in Eq. 9.20, in terms of f(z,0)andf*(z,0)

Short Answer

Expert verified

The expression forAk is12ฯ€โˆซ-โˆžโˆžfz,0+iฯ‰fgz,0e-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.

f0(z,t)=โˆซ-โˆžโˆžA0(k)ei(kz-ฯ‰t)dk.............(1)

Here, kis the propogation vector and ฯ‰is the angular frequency.

02

Determine A0(k) in term of data-custom-editor="chemistry" f (z,0) and data-custom-editor="chemistry" f *(z,0)

Substitute t=0in equation (1).

f0z,0=โˆซ-โˆžโˆžA0keikz-ฯ‰0dk=โˆซ-โˆžโˆžA0keikzdk

Write the conjugate of the above expression.

f0z,0*=โˆซ-โˆžโˆžA0-k*e-ikzdkf0z,0*=โˆซ-โˆžโˆžA0k*e-ikz-dk

It is known that,

fz,0=Ref0z,0fz,0=12f0z,0+f0z,0*....2

Substitute 12A0keikzdkfor f0z,0and 12A0-k*eikzdkfor f0z,0*in equation (2)

fz,0=โˆซ-โˆžโˆž12A0k+A0-k*eikzdk

Substitute fz,0=โˆซ-โˆžโˆž12A0k+A0-k*eikzdkin equation (2).

12A0k+A0-k*=12ฯ€โˆซ-โˆžโˆžfz,0e-ikzdk ......(3)

Solve the conjugate for f0z,0.

f0z,t=โˆซ-โˆžโˆžA0k-iฯ‰eikz-ฯ‰tdkf0z,t=โˆซ-โˆžโˆž-iฯ‰A0keikzdkf0z,t=โˆซ-โˆžโˆžiฯ‰A0keikz-dk

On further solving, the above equation becomes,

fgz,0*=โˆซ-โˆžโˆžiฯ‰Ag-k*e-ikzdkfgz,0=Refgz,0fgz,0=12fgz,0+fgz,0*.......4

Substitute 12-iฯ‰A0keikzdkfor fgz,0and 12-iฯ‰A0k*eikzdkfor fgz,0*in equation (4).

fgz,0=โˆซ-โˆžโˆž12-iฯ‰A0k+iฯ‰A0-keikzdkfgz,0=-iฯ‰2A0k-A0-k*

The inversion theorem for Fourier transformation states that,

fgz,0=12ฯ€โˆซ-โˆžโˆžfgz,0eikzdz

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Most popular questions from this chapter

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

Suppose

E(r,ฮธ,ฯ•,t)=Asinฮธr[cos(krโˆ’ฯ‰t)โˆ’(1/kr)sin(krโˆ’ฯ‰t)]ฯ•^

(This is, incidentally, the simplest possible spherical wave. For notational convenience, let role="math" localid="1658817164296" (krโˆ’ฯ‰t)โ‰กu in your calculations.)

(a) Show that E obeys all four of Maxwell's equations, in vacuum, and find the associated magnetic field.

(b) Calculate the Poynting vector. Average S over a full cycle to get the intensity vector I. (Does it point in the expected direction? Does it fall off likerโˆ’2, as it should?)

(c) Integrate role="math" localid="1658817283737" Iโ‹…da over a spherical surface to determine the total power radiated. [Answer: 4ฯ€A2/3ฮผ0c ]

In writing Eqs. 9.76 and 9.77, I tacitly assumed that the reflected and transmitted waves have the same polarization as the incident waveโ€”along the x direction. Prove that this must be so. [Hint: Let the polarization vectors of the transmitted and reflected waves be

n^T=cosฮธTx^+sinฮธTy^,n^R=cosฮธRx^+sinฮธRy^prove from the boundary conditions that ฮธT=ฮธR=0.]

Show that the mode TE00 cannot occur in a rectangular wave guide. [Hint: In this case role="math" localid="1657512848808" ฯ‰c=k, so Eqs. 9.180 are indeterminate, and you must go back to Eq. 9.179. Show thatrole="math" localid="1657512928835" Bz is a constant, and henceโ€”applying Faradayโ€™s law in integral form to a cross sectionโ€”thatrole="math" localid="1657513040288" Bz=0 , so this would be a TEM mode.]

A microwave antenna radiating at 10โ€„GHzis 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.]

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