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Planar waveguides
Planar waveguides are an important subclass of
waveguides (transmission lines)
Planar waveguides can be used in integrated
circuits to connect the various microwave circuit
elements
Examples are shown in the next three slides
1Falah Mohammed
Applications of planar
waveguides
Also planar transmission lines can be used to
feed microwave energy from a microwave
generator to an antenna as shown
2Falah Mohammed
Applications of planar
waveguides
Planar waveguides can be used to
interconnect the various parts of a
microwave amplifiers
3Falah Mohammed
Applications of planar
waveguides
Planar wave guides also can be used to
design filters and phase shifters
4Falah Mohammed
Filter Phase shifter
Types of planar wave guides
There are many types of planar waveguides
available. Examples are
 Strip line
 Microstrip line
 Coplanar waveguide
 Slotted lines
These waveguides support TEM, TE and TM
wave propagations
However only TEM will be considered
5Falah Mohammed
Planar waveguide design
parameters
When designning a given microwave circuit, it is
desired to know the characteristic impedance,
dispersion curves, phase velocity, phase delay,
capacitance, inductance and the attenuation per unit
length of the waveguide
Computing these parameters can be performed by
solving the Helmholtz equation
However, the computation can be greatly simplified
by the use of commercial microwave design tools
such as CST, AWR microwave office, Agilent ADS,
and HFSS
6Falah Mohammed
Strip-line
The strip line is composed from a thin conducting
strip of width 𝑊 centered between two conducting
ground planes of separation 𝑏
The region between the conducting planes is filled
with a dielectric material whose relative permitivity
is 𝜖 𝑟 as shown
7Falah Mohammed
Strip line
The strip line can be considered as a planar
coaxial cable
Exact solution for the electric field can be
obtained by a method known as conformal
mapping
However this avoided in practice and an
empirical formulas can be used to design the
strip line for specific characteristic impedance
𝑍0, phase velocity 𝑣 𝑝, propagation constant 𝛽
8Falah Mohammed
Formulas for Propagation Constant,
Characteristic Impedance
The phase velocity can be given by
𝑣 𝑝 =
1
𝜇𝜖
=
𝑐
𝜖 𝑟
The propagation constant is given by
𝛽 =
𝜔
𝑣 𝑝
= 𝜔 𝜇0 𝜖0 𝜖 𝑟 = 𝜖 𝑟 𝑘0
The characteristic impedance can be approximated by
𝑍0 =
30𝜋
𝜖 𝑟
𝑏
𝑊𝑒 + 0.441𝑏
Where 𝑊𝑒 is the effective width of the center conductor
which is approximated by
9Falah Mohammed
Strip line width for specific 𝑍0
The strip line width that can be used to design a
strip line with a specific characteristic impedance
can be determined from the following equation
𝑥 =
30𝜋
𝜖 𝑟 𝑍0
− 0.441
10Falah Mohammed
Attenuation due to conductor
loss
11Falah Mohammed
Example
Find the width for a 50 Ω copper stripline
conductor with 𝑏 = 0.32 𝑐𝑚 and 𝜖 𝑟 = 2.2. If the
dielectric loss tangent is 𝑡𝑎𝑛𝛿 = 0.001 and the
operating frequency is 10 GHz, calculate the
attenuation in 𝑑𝐵/𝜆 . Assume a conductor
thickness of 𝑡 = 0.01 mm
12Falah Mohammed
Solution
To find the strip line width we can rely on the
equations in slide 10
𝜖 𝑟 𝑍0 = 2.2 50 = 74.2 < 120
Therefore
𝑥 =
30𝜋
𝜖 𝑟
− 0.441 = 0.83
We can use the equation
𝑊
𝑏
= 𝑥 ⇒ 𝑊 = 𝑏𝑥 = 0.32 × 0.83 = 0.266 𝑐𝑚
13Falah Mohammed
Solution
The total attenuation is the attenuation due to
the conductor loss plus the attenuation due to
dielectric material, therefore
𝛼 = 𝛼 𝑐 + 𝛼 𝑑
𝛼 𝑑 =
𝑘𝑡𝑎𝑛𝛿
2
But
𝑘 = 𝜔 𝜇𝜖 =
2𝜋𝑓 𝜖 𝑟
𝑐
= 310.6
14Falah Mohammed
Solution
Now 𝛼 𝑑 =
310.6×0.001
2
= 0.155 𝑁𝑝/𝑚
The conductor loss can be determined from
The surface resistance for the copper is
𝑅 𝑠
𝜔𝜇
2𝜎
= 0.026 Ω 𝑎𝑡 10 𝐺𝐻𝑧
15Falah Mohammed
Solution
𝛼 𝑐 = 2.6 ×
10−3
𝑅 𝑠 𝜖 𝑟 𝑍0 𝐴
30𝜋(𝑏 − 𝑡)
= 0.122 𝑁𝑝/𝑚
The total attenuation is
𝛼 = 𝛼 𝑑 + 𝛼 𝑐 = 0.277
𝑁𝑝
𝑚
𝛼 𝑑𝐵 = 20 log10 𝑒 𝛼 = 2.41 𝑑𝐵/𝑚
The wavelength at 10 𝐺𝐻𝑧 is
𝜆 =
𝑐
𝜖 𝑟 𝑓
= 2.02 𝑐𝑚
The attenuation in terms of wavelength is
𝛼 𝑑𝐵 = 2.41 × 0.0202 = 0.049 𝑑𝐵/𝜆
16Falah Mohammed
Microstrip line
The microstrip line is one of the most popular
type of transmission lines
The microstrip line is composed from a signal
conductor of width 𝑊 and ground plane
separated by a dielectric material as shown
17Falah Mohammed
Phase velocity, propagation
constant
The phase velocity on microstrip line is given by
𝑣 𝑝 =
𝑐
𝜖 𝑒
The propagation constant is given by
𝛽 = 𝜔 𝜇0 𝜖0 𝜖 𝑒 = 𝑘0 𝜖 𝑒
Where 𝜖 𝑒 is the effective dielectric constant 1 <
𝜖 𝑒 < 𝜖 𝑟
18Falah Mohammed
Effective dielectric constant 𝜖 𝑒
The effective dielectric constant can be
approximated by
𝜖 𝑒 =
𝜖 𝑟 + 1
2
+
𝜖 𝑟 − 1
2
1
1 + 12𝑑/𝑊
19Falah Mohammed
Characteristic impedance
analysis formula
If the dimensions of the microstrip are known, then
the characteristic impedance can be determined
from
20Falah Mohammed
Characteristic impedance
Synthesis formula
If the microstrip is designed to have a specific
characteristic impedance, then the ratio of its width
𝑊 to the dielectric thickness 𝑑 can be determined
form
21Falah Mohammed
Microstrip attenuation
The attenuations for quasi TEM microstrip are
determined from the following two equations
22Falah Mohammed
Example microstrip design
Design a microstrip line on a 0.5 mm alumina
substrate ( 𝜖 𝑟 = 9.9, 𝑡𝑎𝑛 𝛿 = 0.001 ) for a 50 Ω
characteristic impedance.
Find the length of this line required to produce a
phase delay of 270° at 10 GHz, and compute the
total loss on this line, assuming copper
conductors.
23Falah Mohammed
Solution
If we assume that
𝑊
𝑑
< 2, the width 𝑊 can be
determined from
𝑊
𝑑
=
8𝑒 𝐴
𝑒2𝐴 − 2
𝐴 =
𝑍0
60
𝜖 𝑟 + 1
2
+
𝜖 𝑟 − 1
𝜖 𝑟 − 1
0.23 +
0.11
𝜖 𝑟
= 2.142
𝑊/𝑑 = 0.9654 which is less than 2
The required width of microstrip line is 𝑊 =
0.9654𝑑 = 0.483 𝑚𝑚
24Falah Mohammed
Solution
The length of the line that can produce a phase
shift of 𝜙 = 270° can be determined from the
electrical length
𝜖 𝑒 = 6.665
𝜙 = 𝛽𝑙 = 𝜖 𝑒 𝑘0 𝑙 = 270
𝑘0 =
2𝜋𝑓
𝑐
= 209.4 𝑚−1
𝑙 =
270
𝜋
180
𝜖 𝑒 𝑘0
= 8.72 𝑚𝑚
25Falah Mohammed
Solution
By solving for 𝛼 𝑑 and 𝛼 𝑐 , we have a total
attenuation of 𝛼 = 𝛼 𝑑 + 𝛼 𝑐 = 0.022 + 0.094 =
0.116 𝑑𝐵𝑚/𝑐𝑚
The attenuation within the length of the phase
shifter is given by
𝑎𝑡𝑡𝑒𝑛𝑢𝑎𝑡𝑖𝑜𝑛 = 𝛼𝑑𝐵𝑐𝑚 × 𝑙𝑒𝑛𝑔𝑡ℎ 𝑜𝑓 𝑡ℎ𝑒 𝑙𝑖𝑛𝑒
𝑎𝑡𝑡𝑒𝑛𝑢𝑎𝑡𝑖𝑜𝑛 = 0.116 × 0.872 = 0.101 𝑑𝐵
26Falah Mohammed
Coplanar waveguide
The coplanar waveguide is composed
from a central conductor with two ground
planes as shown below
27Falah Mohammed
Coplanar waveguide
The impedance of the coplanar waveguide can
be determined the width of the central conductor
𝑊 and the spacing from the ground planes 𝑆
28Falah Mohammed
Commercial software
The dimensions of planar wave guide can
be adjusted for specific 𝑍0, 𝑣 𝑝, 𝛽, 𝑎𝑛𝑑 𝜙 by
using CAD tool such on line tools or
Linecalc in ADS
29Falah Mohammed
Linecalc
30Falah Mohammed
You can find the line calculator program
under tools, then LineCalc
Starting the line calculator
If you press the start LineCalc item, you may obtain a
window as shown below
31Falah Mohammed
Entering the dielectric parameters
You can enter the
dielectric (substrate)
parameters in the
following section of
the LineCalc window
32Falah Mohammed
Computing
𝑍0, 𝑝ℎ𝑎𝑠𝑒 𝑠ℎ𝑖𝑓𝑡 𝜙 , 𝜖 𝑒 (Analysis)
Enter the width and length of the transmission line and
click on the analyze window, the LineCalc program will
compute 𝑍0, 𝜙, 𝜖 𝑒 as illustrated by
33Falah Mohammed
Computing the 𝑊 and 𝐿 for a
specific 𝑍0 and 𝜙 (Synthesis)
Enter the value of the desired 𝑍0 and the phase shift in
the section provided, press synthesize, the program will
compute the width and length of the transmission line
34Falah Mohammed
Comparison of Common Transmission
Lines and Waveguides
35Falah Mohammed
36Falah Mohammed
Microwave Frequency Bands (taken from wikipedia)
Letter Designation Frequency range
L band 1 to 2 GHz
S band 2 to 4 GHz
C band 4 to 8 GHz
X band 8 to 12 GHz
Ku band 12 to 18 GHz
K band 18 to 26.5 GHz
Ka band 26.5 to 40 GHz
Q band 33 to 50 GHz
U band 40 to 60 GHz
V band 50 to 75 GHz
E band 60 to 90 GHz
W band 75 to 110 GHz
F band 90 to 140 GHz
D band 110 to 170 GHz

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planar wave guide

  • 1. Planar waveguides Planar waveguides are an important subclass of waveguides (transmission lines) Planar waveguides can be used in integrated circuits to connect the various microwave circuit elements Examples are shown in the next three slides 1Falah Mohammed
  • 2. Applications of planar waveguides Also planar transmission lines can be used to feed microwave energy from a microwave generator to an antenna as shown 2Falah Mohammed
  • 3. Applications of planar waveguides Planar waveguides can be used to interconnect the various parts of a microwave amplifiers 3Falah Mohammed
  • 4. Applications of planar waveguides Planar wave guides also can be used to design filters and phase shifters 4Falah Mohammed Filter Phase shifter
  • 5. Types of planar wave guides There are many types of planar waveguides available. Examples are  Strip line  Microstrip line  Coplanar waveguide  Slotted lines These waveguides support TEM, TE and TM wave propagations However only TEM will be considered 5Falah Mohammed
  • 6. Planar waveguide design parameters When designning a given microwave circuit, it is desired to know the characteristic impedance, dispersion curves, phase velocity, phase delay, capacitance, inductance and the attenuation per unit length of the waveguide Computing these parameters can be performed by solving the Helmholtz equation However, the computation can be greatly simplified by the use of commercial microwave design tools such as CST, AWR microwave office, Agilent ADS, and HFSS 6Falah Mohammed
  • 7. Strip-line The strip line is composed from a thin conducting strip of width 𝑊 centered between two conducting ground planes of separation 𝑏 The region between the conducting planes is filled with a dielectric material whose relative permitivity is 𝜖 𝑟 as shown 7Falah Mohammed
  • 8. Strip line The strip line can be considered as a planar coaxial cable Exact solution for the electric field can be obtained by a method known as conformal mapping However this avoided in practice and an empirical formulas can be used to design the strip line for specific characteristic impedance 𝑍0, phase velocity 𝑣 𝑝, propagation constant 𝛽 8Falah Mohammed
  • 9. Formulas for Propagation Constant, Characteristic Impedance The phase velocity can be given by 𝑣 𝑝 = 1 𝜇𝜖 = 𝑐 𝜖 𝑟 The propagation constant is given by 𝛽 = 𝜔 𝑣 𝑝 = 𝜔 𝜇0 𝜖0 𝜖 𝑟 = 𝜖 𝑟 𝑘0 The characteristic impedance can be approximated by 𝑍0 = 30𝜋 𝜖 𝑟 𝑏 𝑊𝑒 + 0.441𝑏 Where 𝑊𝑒 is the effective width of the center conductor which is approximated by 9Falah Mohammed
  • 10. Strip line width for specific 𝑍0 The strip line width that can be used to design a strip line with a specific characteristic impedance can be determined from the following equation 𝑥 = 30𝜋 𝜖 𝑟 𝑍0 − 0.441 10Falah Mohammed
  • 11. Attenuation due to conductor loss 11Falah Mohammed
  • 12. Example Find the width for a 50 Ω copper stripline conductor with 𝑏 = 0.32 𝑐𝑚 and 𝜖 𝑟 = 2.2. If the dielectric loss tangent is 𝑡𝑎𝑛𝛿 = 0.001 and the operating frequency is 10 GHz, calculate the attenuation in 𝑑𝐵/𝜆 . Assume a conductor thickness of 𝑡 = 0.01 mm 12Falah Mohammed
  • 13. Solution To find the strip line width we can rely on the equations in slide 10 𝜖 𝑟 𝑍0 = 2.2 50 = 74.2 < 120 Therefore 𝑥 = 30𝜋 𝜖 𝑟 − 0.441 = 0.83 We can use the equation 𝑊 𝑏 = 𝑥 ⇒ 𝑊 = 𝑏𝑥 = 0.32 × 0.83 = 0.266 𝑐𝑚 13Falah Mohammed
  • 14. Solution The total attenuation is the attenuation due to the conductor loss plus the attenuation due to dielectric material, therefore 𝛼 = 𝛼 𝑐 + 𝛼 𝑑 𝛼 𝑑 = 𝑘𝑡𝑎𝑛𝛿 2 But 𝑘 = 𝜔 𝜇𝜖 = 2𝜋𝑓 𝜖 𝑟 𝑐 = 310.6 14Falah Mohammed
  • 15. Solution Now 𝛼 𝑑 = 310.6×0.001 2 = 0.155 𝑁𝑝/𝑚 The conductor loss can be determined from The surface resistance for the copper is 𝑅 𝑠 𝜔𝜇 2𝜎 = 0.026 Ω 𝑎𝑡 10 𝐺𝐻𝑧 15Falah Mohammed
  • 16. Solution 𝛼 𝑐 = 2.6 × 10−3 𝑅 𝑠 𝜖 𝑟 𝑍0 𝐴 30𝜋(𝑏 − 𝑡) = 0.122 𝑁𝑝/𝑚 The total attenuation is 𝛼 = 𝛼 𝑑 + 𝛼 𝑐 = 0.277 𝑁𝑝 𝑚 𝛼 𝑑𝐵 = 20 log10 𝑒 𝛼 = 2.41 𝑑𝐵/𝑚 The wavelength at 10 𝐺𝐻𝑧 is 𝜆 = 𝑐 𝜖 𝑟 𝑓 = 2.02 𝑐𝑚 The attenuation in terms of wavelength is 𝛼 𝑑𝐵 = 2.41 × 0.0202 = 0.049 𝑑𝐵/𝜆 16Falah Mohammed
  • 17. Microstrip line The microstrip line is one of the most popular type of transmission lines The microstrip line is composed from a signal conductor of width 𝑊 and ground plane separated by a dielectric material as shown 17Falah Mohammed
  • 18. Phase velocity, propagation constant The phase velocity on microstrip line is given by 𝑣 𝑝 = 𝑐 𝜖 𝑒 The propagation constant is given by 𝛽 = 𝜔 𝜇0 𝜖0 𝜖 𝑒 = 𝑘0 𝜖 𝑒 Where 𝜖 𝑒 is the effective dielectric constant 1 < 𝜖 𝑒 < 𝜖 𝑟 18Falah Mohammed
  • 19. Effective dielectric constant 𝜖 𝑒 The effective dielectric constant can be approximated by 𝜖 𝑒 = 𝜖 𝑟 + 1 2 + 𝜖 𝑟 − 1 2 1 1 + 12𝑑/𝑊 19Falah Mohammed
  • 20. Characteristic impedance analysis formula If the dimensions of the microstrip are known, then the characteristic impedance can be determined from 20Falah Mohammed
  • 21. Characteristic impedance Synthesis formula If the microstrip is designed to have a specific characteristic impedance, then the ratio of its width 𝑊 to the dielectric thickness 𝑑 can be determined form 21Falah Mohammed
  • 22. Microstrip attenuation The attenuations for quasi TEM microstrip are determined from the following two equations 22Falah Mohammed
  • 23. Example microstrip design Design a microstrip line on a 0.5 mm alumina substrate ( 𝜖 𝑟 = 9.9, 𝑡𝑎𝑛 𝛿 = 0.001 ) for a 50 Ω characteristic impedance. Find the length of this line required to produce a phase delay of 270° at 10 GHz, and compute the total loss on this line, assuming copper conductors. 23Falah Mohammed
  • 24. Solution If we assume that 𝑊 𝑑 < 2, the width 𝑊 can be determined from 𝑊 𝑑 = 8𝑒 𝐴 𝑒2𝐴 − 2 𝐴 = 𝑍0 60 𝜖 𝑟 + 1 2 + 𝜖 𝑟 − 1 𝜖 𝑟 − 1 0.23 + 0.11 𝜖 𝑟 = 2.142 𝑊/𝑑 = 0.9654 which is less than 2 The required width of microstrip line is 𝑊 = 0.9654𝑑 = 0.483 𝑚𝑚 24Falah Mohammed
  • 25. Solution The length of the line that can produce a phase shift of 𝜙 = 270° can be determined from the electrical length 𝜖 𝑒 = 6.665 𝜙 = 𝛽𝑙 = 𝜖 𝑒 𝑘0 𝑙 = 270 𝑘0 = 2𝜋𝑓 𝑐 = 209.4 𝑚−1 𝑙 = 270 𝜋 180 𝜖 𝑒 𝑘0 = 8.72 𝑚𝑚 25Falah Mohammed
  • 26. Solution By solving for 𝛼 𝑑 and 𝛼 𝑐 , we have a total attenuation of 𝛼 = 𝛼 𝑑 + 𝛼 𝑐 = 0.022 + 0.094 = 0.116 𝑑𝐵𝑚/𝑐𝑚 The attenuation within the length of the phase shifter is given by 𝑎𝑡𝑡𝑒𝑛𝑢𝑎𝑡𝑖𝑜𝑛 = 𝛼𝑑𝐵𝑐𝑚 × 𝑙𝑒𝑛𝑔𝑡ℎ 𝑜𝑓 𝑡ℎ𝑒 𝑙𝑖𝑛𝑒 𝑎𝑡𝑡𝑒𝑛𝑢𝑎𝑡𝑖𝑜𝑛 = 0.116 × 0.872 = 0.101 𝑑𝐵 26Falah Mohammed
  • 27. Coplanar waveguide The coplanar waveguide is composed from a central conductor with two ground planes as shown below 27Falah Mohammed
  • 28. Coplanar waveguide The impedance of the coplanar waveguide can be determined the width of the central conductor 𝑊 and the spacing from the ground planes 𝑆 28Falah Mohammed
  • 29. Commercial software The dimensions of planar wave guide can be adjusted for specific 𝑍0, 𝑣 𝑝, 𝛽, 𝑎𝑛𝑑 𝜙 by using CAD tool such on line tools or Linecalc in ADS 29Falah Mohammed
  • 30. Linecalc 30Falah Mohammed You can find the line calculator program under tools, then LineCalc
  • 31. Starting the line calculator If you press the start LineCalc item, you may obtain a window as shown below 31Falah Mohammed
  • 32. Entering the dielectric parameters You can enter the dielectric (substrate) parameters in the following section of the LineCalc window 32Falah Mohammed
  • 33. Computing 𝑍0, 𝑝ℎ𝑎𝑠𝑒 𝑠ℎ𝑖𝑓𝑡 𝜙 , 𝜖 𝑒 (Analysis) Enter the width and length of the transmission line and click on the analyze window, the LineCalc program will compute 𝑍0, 𝜙, 𝜖 𝑒 as illustrated by 33Falah Mohammed
  • 34. Computing the 𝑊 and 𝐿 for a specific 𝑍0 and 𝜙 (Synthesis) Enter the value of the desired 𝑍0 and the phase shift in the section provided, press synthesize, the program will compute the width and length of the transmission line 34Falah Mohammed
  • 35. Comparison of Common Transmission Lines and Waveguides 35Falah Mohammed
  • 36. 36Falah Mohammed Microwave Frequency Bands (taken from wikipedia) Letter Designation Frequency range L band 1 to 2 GHz S band 2 to 4 GHz C band 4 to 8 GHz X band 8 to 12 GHz Ku band 12 to 18 GHz K band 18 to 26.5 GHz Ka band 26.5 to 40 GHz Q band 33 to 50 GHz U band 40 to 60 GHz V band 50 to 75 GHz E band 60 to 90 GHz W band 75 to 110 GHz F band 90 to 140 GHz D band 110 to 170 GHz