The Solutions of Wave Equation in Cylindrical Coordinatesjuiching/EM Theory-2b.pdf · EMT 93 The...
Transcript of The Solutions of Wave Equation in Cylindrical Coordinatesjuiching/EM Theory-2b.pdf · EMT 93 The...
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EMT 93
The Solutions of Wave Equation in Cylindrical CoordinatesThe Helmholtz equation in cylindrical coordinates is
By separation of variables, assume . We have
.
The only possible solution of the above is
where , and are constants of , and . and satisfy
.The final solution for a give set of , and can be expressed as
,
where is the Bessel function of the form
.The exact values of , , and the forms of the harmonicfunctions and the Bessel function are determined by the boundaryconditions.
In general,
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EMT 94
Note:1. Choose , if included.
2. Choose , if included.3. Choose integer , if the space contain all range of , that is,
.
Likewise, the corresponding solutions for and are asfollow.
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EMT 95
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EMT 96
The Circular Waveguide
1.
a. B. C. where
is the roots of .
b. Cutoff frequency:
c. Wave impedance:
2.
a. B. C. where is the roots of
.
b. Cutoff frequency:
c. Wave impedance:
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EMT 97
3. Always degenerate( ).4. First mode:
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EMT 98
Higher Order Modes of Coaxial Lines
mode B. C.:
mode B. C.:
Dominant: .
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EMT 99
Homework #7 Problem 5.7 Circular wave:Radial Waveguide
Radial wave:
Parallel-plate radial waveguideB. C.: at and
TM to z mode:
TE to z mode:
Phase constant:
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EMT 100
Note:
Wave impedance:
Note: 5.6. For real , are complex function of .7. For , is imaginary, is also imaginary, not
propagation, evanescent.8. First modes: .
a. : predominantly resistiveb. : predominantly reactivec. Dominate mode: . Only and exist. TEM,
transmission-line mode.
Inward wave:
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EMT 101
Outward wave:
Wedge Radial WaveguidesAssume no variation in z.B. C.: at and
TM to z mode:
TE to z mode:
Dominant mode: , only and , TEM, transmission-linemode.
Inward: , Outward:
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EMT 102
The Circular Cavity
TM to z mode ( ):
TE to z mode ( ):
Dominant mode:
1. : . Shorted radial waveguide mode .
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EMT 103
2. : . Shorted circular waveguide mode .
3. If , the second resonance is 1.59 times the first
resonant frequency. For rectangular cavity of small height,1.58.
4. Q of mode:
For the same height-to-diameter ratio, the circular cavity has an 8.3%higher Q than the rectangular cavity. This is to be expected, since thevolume-to-area ratio is higher for a circular cylinder than for a squarecylinder.
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EMT 104
Other Guided Waves
Two dielectric Circular Waveguides
Assume z-directed propagation waves. Hybrid modes exist.In dielectric 1:
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EMT 105
In dielectric 2:
B. Cs.: continues at .
A linear equation of unknowns A, B, C, and D. For not trivialsolution, the determinant must be zero, thus solving and .
Partially filled circular waveguidesMust satisfy: finite at , at , at .
Dielectric-rod waveguides (optical fibers)Must satisfy: finite at , decay for .
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EMT 106
where .Dominant mode: the lowest mode. Zero cut-off frequency.
Coated conductor waveguidesMust satisfy: at , at , decay for .
where .Dominant mode: the lowest TM mode. Zero cut-off frequency.
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EMT 118
Chap 6. Spherical Wave FunctionsSpherical Wave Functions satisfying Helmholtz equation ( ).
: spherical Bessel function.
1. Zero-th order:
2. Higher order: polynomials of times or .
3. Only is finite at .
4. For out-going waves and , use .
Alternatively, for , and can be chosen astwo independently solutions. All solutions have singularity at except with integer. Also, for .
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EMT 119
For TM or TE to z analysis, we have
Alternatively, consider TM or TE to analysis.
Note: does not satisfy Helmholtz equation.Then,
where
The electric and magnetic fields can be computed by
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EMT 120
The Spherical Cavity
For TE to r, choose
B.C.: at . We have
where are the p-th zero of .Similarly, for TM to r, choose
.Then,
where are the p-th zero of .
Resonant frequencies:
Note: .
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EMT 121
The first mode:
Degeneracies:example:
Orthogonality Relationships
From Green’s Identity
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EMT 122
Let,
then,
For
Legendre Polynomial Expansion(Fourier-Legendre Series)Let (assume )
then,
Define tesseral harmonics as
,
then the spherical wave function and can be written as
.We have
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EMT 123
Since
When ,
A two-dimensional Fourier-Legendre series can be obtained for afunction on a spherical surface as
Then,
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EMT 124
Space as a WaveguideTM to r:
Then,
TE to r:
Then,
Note:
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EMT 125
Other Radial WaveguidesConical WaveguideB. C.: Solution space: TM to r:
To satisfy the B. C.,
TE to r:
To satisfy the B. C.,
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EMT 126
Biconical WaveguideB. C.: Solution space:
Since is not included, use for .TM to r:
To satisfy the B. C.,
TE to r:
To satisfy the B. C.,
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EMT 127
Dominant (transmission line) Mode: TEM ( )
Note: gives zero fields and is not chosen.Then,
Wedge Waveguides
B. C.: Solution space: TM ro r:
TE ro r:
No spherical TEM mode, but has cylindrical TEM mode.
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EMT 128
Horn WaveguideTM ro r:
TE ro r:
Biconical Cavity
(Shorted transmission line)
Resonant frequencies:
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EMT 129
Source of Spherical Waves
For a z-directed current source
and
Wave Transformation
Consider a plane wave propagating in z-direction:
Solution space: 1. Independent of : m=0.2. included: .3. included: , n integer.Then,
Differentiate both sides n times at , we have
Also we establish the identity:
Scattering by Spheres
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EMT 130
Assume an x-polarized z-traveling plane wave incidenton a PEC sphere with radius a.Then,
and
.
Using wave transformation, we have
From , be expressed as
Derive from and use the following identity,
.
We have
.
Similarly,
In order to match the boundary condition at , that is,
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EMT 131
The form of the scattered field must be the same as the incident fieldexcept the Bessel functions must represent out-going waves.Therefore,
By applying the B. C., we have
At far field, and only retain , we have
Back-scattered fieldConsider
Calculate effective area by
1. Small : term dominant and
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EMT 132
(Good
approximation for )This is Rayleigh scattering law.
2. Large :
Physical optics approximation.3. Others: resonance region.
Consider the fields scattered by small sphere.Use small argument approximation of Besselfunctions, we have
.
Therefore, dominates. At far field from small sphere,
Comparing above to the field radiated by electric and magneticdipoles, the scattered field is the field of an x-directed electric dipoleand a y-directed magnetic dipole as formulated below:
In general, the scattered field of any small body can be expressed interms of an electric dipole and a magnetic dipole. For a conductingbody, the magnetic dipole may vanish, but the electric dipole alwaysexist.
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EMT 133
Dielectric Sphere
For small dielectric sphere, at far field, the equivalent x-directedelectric dipole and y-directed magnetic dipole are
Also, the field inside the sphere is uniform. This results are the sameas D. C. case. This is called quasi-static approximation.
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EMT 134
Appendix: Legendre Functions
Legendre equation:
where is the Legendre function of order n.Associated Legendre equation:
where is the Legendre function of order n and m and