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SupposeAeiax+Beibx=Ceicx, for some nonzero constants A, B, C, a, b, c, and for all x. Prove that a = b = cand A + B = C.

Short Answer

Expert verified

It is proved A + B = C and a = b = c.

Step by step solution

01

Expression for the amplitude and Euler equation:

Write the expression for the amplitude equation.

Aeiax+beibx=Ceicx …… (1)

Write the expression for the Euler equation.

eiθ=cosθ+isinθ

02

Prove A + B = C :

Substitute the known values in equation (1).

A(cosax+isinax)+B(cosbx+isinbx)=C(coscx+isincx)

Write the real part of the equation.

role="math" localid="1657520367793" Acosax+Bcosbx=Ccoscx

Write the real imaginary of the equation.

Asinax+Bsinbx=Csincx

Using boundary conditions at x = 0 , the left-hand side function will be equal to the right-hand side function.

Aeia(0)+Beib(0)=Ceic(0)A+B=C

03

Prove a = b = c :

Square and add the equation (2) and (3).

(Acosax+Bcosbx)2+(Asinax+Bsinbx)2=C2(cos2cx+sin2cx)

Since, cos2cx+sin2cx=1.

On further solving,

A2cos2ax+B2cos2bx+2AB(cosAx)(cosbx)+A2sin2ax+B2sinbx+2AB(sinax)(sinbx)=C2A2(cos2ax+sin2ax+B2(cos2bx+sin2bx)+2AB(cosaxcosbx+sinaxsinbx)=C2A2+B2+2ABcos(a-b)x=C2

Substitute the value of A+B=Cin the above expression.

A2+B2+2ABcos(a-b)x=(A+B)2 A2+B2+2ABcos(a-b)x=A2+B2+2AB2ABcos(a-b)x=2ABcos(a-b)x=1

Hence,

a = b

Substitute the value of a and b in equation (1).

eiax(A+B)=Ceicxeiax(A+B)=(A+B)eicxeiax=eicx

Solve further as,

a = b

= c

Therefore, it is proved A + B = C and a = b = c.

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Most popular questions from this chapter

[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).

Consider a particle of charge q and mass m, free to move in the xyplane in response to an electromagnetic wave propagating in the z direction (Eq. 9.48—might as well set δ=0)).

(a) Ignoring the magnetic force, find the velocity of the particle, as a function of time. (Assume the average velocity is zero.)

(b) Now calculate the resulting magnetic force on the particle.

(c) Show that the (time) average magnetic force is zero.

The problem with this naive model for the pressure of light is that the velocity is 90°out of phase with the fields. For energy to be absorbed there’s got to be some resistance to the motion of the charges. Suppose we include a force of the form ymv, for some damping constant y.

(d) Repeat part (a) (ignore the exponentially damped transient). Repeat part (b), and find the average magnetic force on the particle.

Find all elements of the Maxwell stress tensor for a monochromatic plane wave traveling in the z direction and linearly polarized in the x direction (Eq. 9.48). Does your answer make sense? (Remember that -Trepresents the momentum flux density.) How is the momentum flux density related to the energy density, in this case?

Work out the theory of TM modes for a rectangular wave guide. In particular, find the longitudinal electric field, the cutoff frequencies, and the wave and group velocities. Find the ratio of the lowest TM cutoff frequency to the lowest TE cutoff frequency, for a given wave guide. [Caution: What is the lowest TM mode?]

(a) Suppose you imbedded some free charge in a piece of glass. About how long would it take for the charge to flow to the surface?

(b) Silver is an excellent conductor, but it’s expensive. Suppose you were designing a microwave experiment to operate at a frequency of1010Hz. How thick would you make the silver coatings?

(c) Find the wavelength and propagation speed in copper for radio waves at role="math" localid="1655716459863" 1MHz. Compare the corresponding values in air (or vacuum).

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