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

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

If you take the model in Ex. 4.1 at face value, what natural frequency do you get? Put in the actual numbers. Where, in the electromagnetic spectrum, does this lie, assuming the radius of the atom is 0.5 Å? Find the coefficients of refraction and dispersion, and compare them with the measured values for hydrogen at 0°Cand atmospheric pressure:A=1.36×10-4,B=7.7×10-15m2 .

[The naive explanation for the pressure of light offered in section 9.2.3 has its flaws, as you discovered if you worked Problem 9.11. Here's another account, due originally to Planck.] A plane wave travelling through vaccum in the z direction encounters a perfect conductor occupying the region z0, and reflects back:

E(z,t)=E0[coskz-ωt-coskz+ωt]x^,(z>0)

  1. Find the accompanying magnetic field (in the region (z>0))
  2. Assuming B=0inside the conductor find the current K on the surface z=0, by invoking the appropriate boundary condition.
  3. Find the magnetic force per unit area on the surface, and compare its time average with the expected radiation pressure (Eq.9.64).

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

By explicit differentiation, check that the functions f1, f2, and f3in the text satisfy the wave equation. Show that f4and f5do not.

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.]

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free