Question: Use Eq. 9.19 to determineA3andδ3in terms ofrole="math" localid="1653473428327" A1,A2,δ1, andδ2.

Short Answer

Expert verified

The value of A3is role="math" localid="1653473609796" A3=A12+A22+2A1A2cosδ1-δ2, and the value of δ3 isδ3=tan-1A1sinδ1+A2sinδ2A1cosδ1+A2cosδ2

Step by step solution

01

Expression for the amplitude equation 9.19:

Write the amplitude equation 9.19.

A3eiδ3=A1eiδ1+A2eiδ2

It is known that eiθ=cosθ+isinθ. So, the equation (1) becomes,

A3cosδ3+isinδ3=A1cosδ1+isinδ1+A2cosδ2+isinδ2

02

Determine the value of :

Solve for the real term.

A3cosδ3=A1cosδ1+A2cosδ2 ….. (2)

Solve for the imaginary term.

A3sinδ3=A1sinδ1+A2sinδ2 ….. (3)

Squaring equations (2) and (3) and add them.

A32cos2δ3+A32sin2δ3=A1cosδ1+A2cosδ22+A1sinδ1+A2sinδ22A32cos2δ3+sin2δ3=A1cosδ1+A2cosδ22+A1sinδ1+A2sinδ22A32=A1cosδ1+A2cosδ22+A1sinδ1+A2sinδ22A32=A12cos2δ1+A22cos2δ2+2A1A2cosδ1cosδ2+A12sin2δ1+A22sin2δ2+2A1A2sinδ1sinδ2

Simplify further.

A32=A12cos2δ1+sin2δ1+A22cos2δ2+sin2δ2+2A1A2cosδ1cosδ2+sinδ1sinδ2A32=A121+A221+2A1A2cosδ1-δ2A32=A12+A22+2A1A2cosδ1-δ2A3=A12+A22+2A1A2cosδ1-δ2

Therefore, the value of A3is A3=A12+A22+2A1A2cosδ1-δ2.

03

Determine the value of δ3 :

Divide equation (3) by (2).

A3sinδ3A3cosδ3=A1sinδ1+A1sinδ2A1cosδ1+A1cosδ2tanδ3=A1sinδ1+A1sinδ2A1cosδ1+A1cosδ2δ3=tan-1A1sinδ1+A1sinδ2A1cosδ1+A1cosδ2

Therefore, the value of δ3is δ3=tan-1A1sinδ1+A1sinδ2A1cosδ1+A1cosδ2.

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Most popular questions from this chapter

In the complex notation there is a clever device for finding the time average of a product. Suppose f(r,t)=Acos(k×r-ωt+δa)and g(r,t)=Bcos(k×r-ωt+δb). Show that <fg>=(1/2)Re(fg~), where the star denotes complex conjugation. [Note that this only works if the two waves have the same k andω, but they need not have the same amplitude or phase.] For example,

<u>=14Re(ε0E~×E~+1μ0B~×B~)and<S>=12μ0Re(E~×B).~ and .

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.]

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.]

Confirm that the energy in theTEmnmode travels at the group velocity. [Hint: Find the time-averaged Poynting vector <S>and the energy density <u>(use Prob. 9.12 if you wish). Integrate over the cross-section of the waveguide to get the energy per unit time and per unit length carried by the wave, and take their ratio.]

(a) Show directly that Eqs. 9.197 satisfy Maxwell’s equations (Eq. 9.177) and the boundary conditions (Eq. 9.175).

(b) Find the charge density, λ(z,t), and the current, I(z,t), on the inner conductor.

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