This document discusses different types of waveguides, including rectangular waveguides, circular waveguides, coaxial lines, optical waveguides, and parallel-plate waveguides. It describes the different modes of wave propagation including TEM, TE, TM, and HE modes. Cutoff frequencies and wavelengths are defined for rectangular and parallel-plate waveguides. Dominant TE10 mode is described for rectangular waveguides.
4. ๏ Transverse Electro Magnetic (TEM) wave:
Here both electric and magnetic fields are directed
components. (i.e.) E z = 0 and Hz = 0
๏ Transverse Electric (TE) wave: Here only the electric field is purely transverse to the direction
of propagation and the magnetic field is not purely transverse. (i.e.) E z = 0, Hz โ 0
๏ Transverse Magnetic (TM) wave: Here only magnetic field is transverse to the direction of
propagation and the electric field is not purely transverse. (i.e.) E z โ 0, Hz = 0.
๏ Hybrid (HE) wave: Here neither electric nor magnetic fields are purely transverse to the
direction of propagation. (i.e.) E z โ 0, Hz โ 0.
4
Types of Modes
JIT
5. Transmission line
๏ฑ Voltage applied between conductors(E: vertically between
the conductors)
๏ฑ Interior fields: TEM (Transverse ElectroMagnetic) wave
(wave vector indicates the direction of wave propagation
as well as the direction of power flow)
1. Waveguide
JIT 5
6. Waveguide
๏ฑ A waveguide is a structure that guides waves, such
as electromagnetic waves or sound waves They enable a signal to
propagate with minimal loss of energy by restricting expansion to
one dimension or two
๏ฑ Zigzag reflection, waveguide mode, cutoff frequency
๏ญ๏ฅ๏ท๏ฝ๏ฝ๏ฝ k|||| du kk
JIT 6
8. The electric and magnetic wave equations in frequency
domain is given by
๐ป2
๐ธ = ๐พ2
๐ธ
๐ป2
๐ป = ๐พ2
๐ป
๐พ2
= ๐๐๐(๐ + ๐๐๐)
For a loss less dielectric or perfect conductor
๐พ2
= โ๐2
๐๐
The above equations are like Helmholtz equations
๐ป2
๐ธ๐ง๐ = ๐พ2
๐ธ๐ง๐
Let ๐ธ๐ง๐ =X(x).Y(y).Z(z)
Be the solution of above equations
JIT 8
9. Contโd
So separation equation
-๐ ๐ฅ
2
โ๐ ๐ฆ
2
โ๐ ๐ง
2
= ๐พ2
On Solving the above equations
๐ธ๐ง๐ = ๐ด. sin ๐ ๐ฅ. ๐ฅ + ๐ต. cos(๐ ๐ฅ. ๐ฅ) ร ๐ถ. sin ๐ ๐ฆ. ๐ฆ + ๐ท. cos(๐ ๐ฆ. ๐ฆ)
ร ๐ธ. sin ๐ ๐ง. ๐ง + ๐น. cos(๐ ๐ง. ๐ง)
The propagation of wave in guide is conventionally assumed in +ve Z
direction.
JIT 9
10. Here the propagation constant ๐พ๐ in guide differs from intrinsic
propagation constant ๐พ
Let ๐พ๐
2 = ๐พ 2 + ๐ ๐ฅ
2
+ ๐ ๐ฆ
2
And ๐พ๐
2
= ๐พ 2
+ ๐ ๐
2
Where ๐ ๐= ๐ ๐ฅ
2
+ ๐ ๐ฆ
2
is cutoff wave number.
For a lossless dielectric ๐พ2 = โ๐2 ๐๐
So ๐พ๐= ยฑ๐ ๐2 ๐๐ โ ๐ ๐
2
So there are three casesโฆ.
JIT 10
Contโd
11. Case 1
If ๐2
๐๐ = ๐ ๐
2
๐พ๐= 0 no propagation
This is critical condition for cutoff propagation
๐๐=
1
๐๐
๐ ๐ฅ
2
+ ๐ ๐ฆ
2
๐๐=
1
2๐ ๐๐
๐ ๐ฅ
2
+ ๐ ๐ฆ
2
JIT 11
12. JIT 12
Case 2
If ๐2
๐๐ > ๐ ๐
2
๐พ๐= ยฑ๐๐ฝ๐ = ยฑ๐๐ ๐๐ 1 โ
๐๐
๐
2
This shows that operating frequency should be greater than critical
frequency to propagate the wave in wave in wave guide
13. JIT 13
Case 3
If ๐2
๐๐ < ๐ ๐
2
๐พ๐= ยฑ๐ผ ๐ = ยฑ๐ ๐๐
๐๐
๐
2
โ 1
This shows that if operating frequency is below the cutoff frequency the
wave will decay exponentially wrt a factor -๐ผ ๐ ๐ง and there will no wave
propagation
There for the solution of Helmholtz equation in rectangular co-ordinates
is given by
๐ธ๐ง๐ = ๐ด. sin ๐ ๐ฅ. ๐ฅ + ๐ต. cos(๐ ๐ฅ. ๐ฅ) ร ๐ถ. sin ๐ ๐ฆ. ๐ฆ + ๐ท. cos(๐ ๐ฆ. ๐ฆ)
ร ๐โ๐๐ฝ
14. Rectangular waveguide
๏พ ๏ฑ WR (Waveguide Rectangular) series
- EIA (Electronic Industry Association) designation
WR-62
- Size: 1.58 cmx0.79 cm
- Recommended range: 12.4-18.0 GHz
- Cutoff: 9.486 GHz
2/
cm/10054262inch/10062
ab
.a
๏ป
๏ด๏ฝ๏ฝ
๏พ
JIT 14
15. Waveguide modes
๏ฑ TE (Transverse Electric) mode
- E parallel to the transverse plane of the waveguide
- In waveguide Wave propagates in +ve Z direction
- TEmn in characterized by Ez=0
- In other words the z component of magnetic field must exist
in order to have energy transmission in the guide.
๏ฑ TM (Transverse Magnetic) mode
- H is within the transverse plane of the waveguide
JIT 15
16. TE modes in rectangular waveguides
๐ป2 ร ๐ธ๐ = โ๐๐๐๐ป๐
๐ป2 ร ๐ป๐ = โ๐๐๐๐ธ๐
Therefore the magnetic field in +ve Z direction ie. The solution of above
partial differential equations
H0z is the amplitude constant, so field equations in rectangular
waveguides
JIT 16
mode:)sin()sin(),(
mode:)cos()cos(),(
mn
zj
nmz
mn
zj
nmz
TMeybxayxE
TEeybxayxH
mn
mn
๏ข
๏ข
๏ญ
๏ญ
๏ฝ
๏ฝ
222
and,,where nmmnnm bak
b
n
b
a
m
a ๏ญ๏ญ๏ฝ๏ฝ๏ฝ ๏ข
๏ฐ๏ฐ
zj
nmzz
mn
eybxaHH ๏ข๏ญ
๏ฝ )cos()cos(0
18. TE and TM modes
๏พ ๏ฑ Hz and Ez fields: TE and TM modes
๏ฑ Non-TEM modes: Hz = Ez = 0
๏ฑ Concept of a dominant mode: TE10 mode
mode:)sin()sin(),(
mode:)cos()cos(),(
mn
zj
nmz
mn
zj
nmz
TMeybxayxE
TEeybxayxH
mn
mn
๏ข
๏ข
๏ญ
๏ญ
๏ฝ
๏ฝ
Boundary condition enforcements
: PEC (Perfect Electric Conductor)
222
and,,where nmmnnm bak
b
n
b
a
m
a ๏ญ๏ญ๏ฝ๏ฝ๏ฝ ๏ข
๏ฐ๏ฐ
3. Waveguide
JIT 18
19. Cutoff wave no kc = ๐ ๐ฅ
2
+ ๐ ๐ฆ
2
Where ๐ ๐ฅ=๐ ๐ and ๐ ๐ฆ=๐ ๐
kc =
๐๐
๐
2
+
๐๐
๐
2
= ๐๐ ๐๐
fc =
1
๐๐
๐๐
๐
2
+
๐๐
๐
2
Propagation constant as discussed earlier
๐พ๐= ยฑ๐ ๐2 ๐๐ โ ๐ ๐
2
So from case-1 and case-2 propagation constant or phase constant
๐ฝ๐ = ๐ ๐๐ 1 โ
๐๐
๐
2
JIT 19
28. TE mode representation
๏จ ๏ฉ ๏จ ๏ฉ
๏จ ๏ฉ
waves.planedownwardandupwardtheof
ionsuperpositthefromresultingpatternceinterferentheisfieldmodeTEThe
cutoff)abovemode(TE
)cos(sin)Re(),(
sinsin2)(
,and
'
0
'
000
r
0
r
0
ztxkEeEtzE
exkEexkjEeeeEE
zxkk
eEeEE
mm
tj
ysy
zj
m
zj
m
zjxjkxjk
ys
zxzmxmzmxm
jj
ys
mmmmm
๏ข๏ท
๏ข๏ข
๏ท
๏ข๏ข๏ข
๏ญ๏ฝ๏ฝ
๏ฝ๏ฝ๏ญ๏ฝ
๏ซ๏ฝ๏ซ๏ญ๏ฝ๏ซ๏ฝ
๏ญ๏ฝ
๏ญ๏ญ๏ญ๏ญ
๏ท๏ญ๏ท๏ญ
aaraakaak du
kk du
2. Parallel-plate
JIT 28
29. ๏จ ๏ฉ ๏จ ๏ฉ
)cutoffbelowmodeTE(
)cos(sin),(andsin
1
2
1,If
'
0
'
0
22
texkEtzEexkEE
n
c
n
j
z
my
z
mys
cm
cmcm
cm
mmcm
mm
๏ท
๏ฌ
๏ฌ
๏ฌ
๏ฐ
๏ท
๏ท๏ท
๏ข๏ก๏ท๏ท
๏ก๏ก ๏ญ๏ญ
๏ฝ๏ฝ
๏ท
๏ธ
๏ถ
๏ง
๏จ
๏ฆ
๏ญ๏ฝ๏ท๏ท
๏ธ
๏ถ
๏ง๏ง
๏จ
๏ฆ
๏ญ๏ฝ๏ฝ๏ผ
TE mode representation
infinity.approachesas90gapproachin
increases,anglewavethe,decreased)isor(cutoffbeyondincreasedisAs
guide.down theprogressforwardnomakingarethey
forth;andbackreflectingjustarewavesplanetheand0),(cutoffAt
o
cm
๏ท
๏ฌ๏ท
๏ฑ๏ท๏ท ๏ฝ๏ฝ m
cm
cm
m
๏ฌ
๏ฌ
๏ท
๏ท
๏ฑ ๏ฝ๏ฝcos
2. Parallel-plate
JIT 29
30. Phase and group velocity
mm
c
n
k ๏ฑ
๏ท
๏ฑ๏ข sinsinm ๏ฝ๏ฝ
m
pm
n
c
v
๏ฑ๏ข
๏ท
sin
velocityPhase
m
๏ฝ๏ฝ
m
cm
m
gm
n
c
n
c
d
d
v ๏ฑ
๏ท
๏ท
๏ข
๏ท
sin1:velocityGroup
2
๏ฝ๏ท
๏ธ
๏ถ
๏ง
๏จ
๏ฆ
๏ญ๏ฝ๏ฝ
.relativityspecialaofprincipletheenot violat:
mediumin thelightofspeedtheexceedmayThis
2. Parallel-plate
JIT 30
31. Field analysis
cnkk /where22
๏ท๏ฝ๏ญ๏ฝ๏ ss EE
):variation-,0(0
)ofcomponenta(onlymodesTE
2
2
2
2
2
2
2
2
2
zj
ysysysysys
m
ezE
y
EkE
z
E
y
E
x
y
๏ข๏ญ
๏ฝ
๏ถ
๏ถ
๏ฝ๏ซ
๏ถ
๏ถ
๏ซ
๏ถ
๏ถ
๏ซ
๏ถ
๏ถ
E
zj
mys
m
exfEE ๏ข๏ญ
๏ฝ )(0
0)()(
)( 2
2
2
2
๏ฝ๏ญ๏ซ xfk
dx
xfd
mm
m
๏ข 0)(
)(
, 2
2
2
22
2 ๏ฝ๏ซ๏ฝ๏ญ xfk
dx
xfd
kk mm
m
mm๏ข
๏ท
๏ธ
๏ถ
๏ง
๏จ
๏ฆ
๏ฝ๏ฎ๏ฝ๏ฝ
๏ซ๏ฝ
d
xm
xfdxxE
xkxkxf
my
mmm
๏ฐ
sin)(.and0atzerobemust:BC
),sin()cos()(
๏พ
๏พ
2. Parallel-plate
JIT 31
32. Characteristics of TE mode
cavityresonantldimensionaOne
2
sinsincutoff,At
2
2
cutoff,At/2and0
.2isshiftphasetrip-roundNet
walls.conductingebetween thdownandupbouncessimplywaveThe
zero.isguidein theincidenceofanglewaveplanethecutoff,At
00 ๏ท๏ท
๏ธ
๏ถ
๏ง๏ง
๏จ
๏ฆ
๏ฝ๏ฝ๏ท
๏ธ
๏ถ
๏ง
๏จ
๏ฆ
๏ฝ
๏ฝ๏๏ฝ๏๏ฝ๏ฝ๏ฝ
cm
ysys
cm
cm
cmmm
xn
EE
d
xm
EE
n
m
d
n
d
m
nkk
m
๏ฌ
๏ฐ๏ฐ
๏ฌ
๏ฌ
๏ฐ๏ฐ
๏ฌ๏ฐ๏ข
๏ฐ
zj
ys
m
e
d
xm
EE ๏ข๏ฐ ๏ญ
๏ท
๏ธ
๏ถ
๏ง
๏จ
๏ฆ
๏ฝ sin0๏พ
2. Parallel-plate
JIT 32
34. ๏จ ๏ฉ ๏จ ๏ฉ
๏จ ๏ฉ1cossinand
)(cos)(sin||
||
22222
00222/1220
**
๏ฝ๏ซ๏ฝ๏ซ
๏ฝ๏ฝ๏ซ๏ซ๏ฝ
๏ซ๏ฝ๏ท๏ฝ
AAkk
EkE
xkxkk
E
HHHH
mm
mmmm
zszsxsxsxs
*
๏ข
๏จ๏ท๏ญ
๏ข
๏ท๏ญ
๏
s
sss
H
HHH
Intrinsic impedance
๏พ
2. Parallel-plate
JIT 34
35. Circular waveguide
๏พ ๏ฑ WC (Waveguide Circular) series
๏ฑ Hz and Ez fields: TE and TM modes
3. Waveguide
JIT 35
36. JIT 36
๏ A microstrip is constructed with a flat conductor suspended over a ground
plane. The conductor and ground plane are separated by a dielectric.
๏ The surface microstrip transmission line also has free space (air) as the
dielectric above the conductor.
๏ This structure can be built in materials other than printed circuit boards,
but will always consist of a conductor separated from a ground plane by
some dielectric material.
Microstrip transmission line
4. Tx line
37. Circular waveguide
๏Circular waveguides offer implementation advantages
over rectangular waveguide in that installation is much simpler.
๏When forming runs for turns and offsets - particularly when large radii
are involved - and the wind loading is less on a round cross-section,
meaning towers do not need to be as robust.
JIT 37
38. For a circular waveguide of radius a,
we can perform the same sequence
of steps in cylindrical coordinates as
we did in rectangular coordinates to
find the transverse field components
in terms of the longitudinal (i.e. Ez,
Hz) components.
JIT 38
39. The scalar Helmholtz equation in cylindrical co-ordinate is given by
Using the method of separation of variables, the solution of above equation
is assumed
๐น = ๐ ๐ . โ โ . ๐ ๐ง โโโโ โ(1)
Substituting (1) into (a) and solving this equation for
๐ ๐ , โ โ ๐๐๐ ๐ ๐ง
So here also
๐ ๐
2
+ ๐พ2
= ๐พ๐
2
This is also called as characteristic equation of Besselโs equations.
For a lossless guide
๐ฝ๐ = ยฑ ๐2 ๐๐ โ ๐ ๐
2
JIT 39
(a)
40. The total solution of Helmholtz equation in cylindrical co-ordinate
JIT 40
41. TE Modes in Circular Waveguides
It is commonly assumed that the waves in a circular waveguide are
propagating in the positive z direction. Here in this mode ๐ธ๐ง = 0, so
๐ธ ๐ฅ, ๐ธ ๐ฆ, ๐ป ๐ฅ, ๐ป ๐ฆ ๐๐๐ ๐ป๐ง.
After substituting boundary conditions the final solution is
๐น = ๐น0. ๐ฝ ๐ ๐ ๐. ๐ cos ๐โ . ๐โ๐๐ฝ ๐ ๐ง
For a lossless dielectric, Maxwellโs equations
๐ป ร ๐ธ = โ๐๐๐๐ป๐
๐ป ร ๐ป = ๐๐๐๐ธ๐
JIT 41
43. When the differentiation ๐/๐๐ง is replaced by (โ๐๐ฝ๐)and the z
component ๐ธ๐ง by zero, the TE mode equations in terms of ๐ป๐งin
circular waveguide are expressed as ๐ธ ๐ = 0
JIT 43
Where ๐ ๐
2
= ๐2 ๐๐ โ ๐ฝ๐
44. The permissible value of kc can be written as
๐ ๐ =
๐ ๐๐
โฒ
๐
Where ๐ ๐๐
โฒ
is a constant
And from above table ๐ ๐๐
โฒ
=1.841 for TM11 MODE
JIT 44
46. ๏Where Zg = Er/ ๐ปโ , = - ๐ธโ / Hr has been replaced for the wave
impedance in the guide and where n = 0,1,2,3,... And p = 1, 2, 3, 4,....
๏The first subscript n represents the number of full cycles of field
variation in one revolution through 2๐ rad of โ .
๏The second subscript p indicates the number of zeroes of ๐ธโ .
๏The mode propagation constant is determined by
๐ฝ๐ = ยฑ ๐2 ๐๐ โ
๐ ๐๐
โฒ
๐
JIT 46
47. The cutoff wave number of a mode is that for which the mode
propagation constant vanishes. Hence
๐ ๐ =
๐ ๐๐
โฒ
๐
= ๐๐ ๐๐
So
๐๐ =
๐ ๐๐
โฒ
2๐๐ ๐๐
And the phase velocity for TE modes is
๐ฃ๐ =
๐
๐ฝ๐
=
๐ฃ ๐
1 โ
๐๐
๐
2
๐คโ๐๐๐ ๐ฃ ๐ =
1
๐๐
=
๐
๐ ๐ ๐ ๐
JIT 47
48. The wavelength and wave impedance for TE modes in a circular guide
are given, respectively, by
JIT 48
๐ ๐ =
๐ฌ ๐
๐ฏ ๐
=
49. TM Modes in Circular Waveguides
The TMnp modes in a circular guide are characterized by Hz = 0.
However, the z component of the electric field E, must exist in order to
have energy transmission in the guide.
Consequently, the Helmholtz equation for Ez in a circular waveguide is
given by
Its solution is given in Eq.
Which is subject to the given boundary conditions.
JIT 49
(A)
51. Similarly
On differentiating equation (A) wrt z and substituting the result in
above equations yield the field equations of TMnp modes in a
circular waveguide:
JIT 51
53. Some of the TM-mode characteristic equations in the circular guide
are identical to those of the TE mode, but some are different. For
convenience, all are shown here:
JIT 53
54. It should be noted that the dominant mode, or the mode
of lowest cutoff frequency in a circular waveguide, is
the mode of TEnp that has the smallest value of the
product, kc .a = 1. 841, as shown in above Table.
JIT 54