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Show that the modeTE00 cannot occur in a rectangular wave guide. [Hint: In this caseωc=k , so Eqs. 9.180 are indeterminate, and you must go back to Eq. 9.179. Show that is a constant, and hence—applying Faraday’s law in integral form to a cross section—thatBz=0 , so this would be a TEM mode.]

Short Answer

Expert verified

It is proved that the TE00mode cannot occur in a rectangular waveguide.

Step by step solution

01

Determine the electric field in y-direction:

  • First equation:

Write the expression for Maxwell’s equation.

Ezy-iKEy=iωBx …… (1)

For a rectangular waveguide, asωc=k and Ez=0then, equation (1) becomes,

(0)yiωcEy=iωBxEy=cBx

  • Second Maxwell’s equation:

Write the expression for Maxwell’s equation.

ikEx-Ezx=iωBy …… (2)

  • Third Maxwell’s equation:

Write the expression for Maxwell’s equation.

Bzy-ikBy=-iωc2Ex …… (3)

  • Fourth Maxwell’s equation:

Write the expression for Maxwell’s equation.

ikBx-Bzx=-iωc2Ey …… (4)

02

Show that the mode cannot occur in a rectangular guide wave.

Substitutek=ωcand Ezx=0in the equation (2).

iωcEx0=iωByEx=cBy

Substitute Ex=cByin the equation (3).

BzyikBy=iωc2(cBy)Bzy=ikByikByBzy=0

SubstituteEy=cBxin the equation (4).

ikBxBzx=iωc2(cBx)ikBxBzx=ikBxBzx=0

Hence,

Bzx=Bzy=0

If the boundary is just inside the metal, the value of E will be zero. So, the value of B will also be zero.

Hence, this is a TEM mode, and TE00mode cannot occur in a rectangular waveguide.

Therefore, the TE00mode cannot occur in a rectangular waveguide.

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Most popular questions from this chapter

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?

The "inversion theorem" for Fourier transforms states that

ϕ(Z)=-ϕ(k)eikzdkϕ(k)=12π-ϕ(z)e-ikzdz

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

Suppose

E(r,θ,ϕ,t)=Asinθr[cos(krωt)(1/kr)sin(krωt)]ϕ^

(This is, incidentally, the simplest possible spherical wave. For notational convenience, let role="math" localid="1658817164296" (krωt)u 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 liker2, as it should?)

(c) Integrate role="math" localid="1658817283737" Ida over a spherical surface to determine the total power radiated. [Answer: 4πA2/3μ0c ]

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

n^T=cosθTx^+sinθTy^,n^R=cosθRx^+sinθRy^prove from the boundary conditions that θT=θR=0.]

Show that the mode TE00 cannot occur in a rectangular wave guide. [Hint: In this case role="math" localid="1657512848808" ωc=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 hence—applying Faraday’s law in integral form to a cross section—thatrole="math" localid="1657513040288" Bz=0 , so this would be a TEM mode.]

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