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Lecture #3
Microstrip lines
Instructor:
Dr. Ahmad El-Banna
Benha University
Faculty of Engineering at Shoubra
November
2014
Post-Graduate
ECE-601
Active Circuits
©
Ahmad
El-Banna
Agenda
Striplines
Forward & Reverse Striplines Design
Microstrip lines
Design of Microstrip lines
Multi-layer Microstrip lines 2
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
STRIPLINES 3
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
Stripline Transmission Lines
• Microwave circuits that supports TEM or “quasi-TEM”
modes are:
• Microstrip and covered microstrip
• Stripline
• Slotline
• Coplanar waveguide.
• Stripline has one or more interior strip conductors immersed
in a dielectric with ground planes above and below.
4
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
Formulasfor PropagationConstant,
CharacteristicImpedance,and Attenuation
• Stripline can support the TEM mode exclusively provided
that
• At higher frequencies, TE and TM modes may also propagate,
which leads to signal distortion and other undesirable
effects. This is called an “over-moded” waveguide.
• We’ll assume that the (carrier) frequency is “low” enough
that and only the TEM mode propagates. As with
any TEM mode, in a stripline with
5
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
none of these quantities depend
on frequency for a TEM mode.
propagation constant
characteristic
impedance of a
transmission line
phase velocity
FORWARD & REVERSE STRIPLINES
DESIGN
6
ECE-601
,
Lec#3
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Nov
2014
©
Ahmad
El-Banna
Forward Stripline Design
• We will need to design stripline with a specific Z0.
• Determining the C value is the problem. There is no simple,
exact analytical solution for stripline (or microstrip, for that matter).
• But extremely accurate numerical solutions can be found using a
number of techniques including the method of moments and the
finite element method, among others.
• By curve fitting to these numerical solutions, it can be shown
that for a stripline:
7
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
where We is called an “effective strip width” given by
*These formulas assume a strip with zero
thickness and are quoted as being
accurate to about 1% of the exact results.
Reverse Stripline Design
• One can determine the “inverse” of Z0, so that W/ b can
be determined once εr and the required Z0 are specified:
•
8
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
MICROSTRIP LINES 9
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
Microstrip lines
• One of the most widely used planar microwave
circuit interconnections is microstrip. These are commonly
formed by a strip conductor (land) on a dielectric substrate,
which is backed by a ground plane.
• We will often assume the land has zero thickness, t.
• In practical circuits there will often be metallic walls and
covers to protect the circuit. We will ignore these effects.
• Unlike stripline, a microstrip has more than one dielectric
in which the EM fields are located.
• This presents a difficulty. 10
ECE-601
,
Lec#3
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Nov
2014
©
Ahmad
El-Banna
Microstrip lines..
• If the field propagates as a TEM wave, then
• But which εr do we use?
• The answer is neither because there is actually no purely TEM wave
on the microstrip, but something that closely approximates it called
a “quasi-TEM” mode.
• At low frequency, this mode is almost exactly TEM.
• Conversely, when the frequency becomes too high, there are axial
components of E and/or H making the mode no longer quasi-TEM.
• This property leads to dispersive behavior.
• Numerical and other analysis have been performed on microstrip
since approximately 1965.
• Some techniques, such as the method of moments, produce very
accurate numerical solutions to equations derived directly from
Maxwell’s equations and incorporate the exact cross-sectional
geometry and materials of the microstrip.
11
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
Microstrip lines…
• From these solutions, simple and quite accurate analytical
expressions for Z0, ʋp etc. have been developed primarily by
curve fitting.
• The result of these analyses is that at relatively “low” frequency, the
wave propagates as a quasi-TEM mode with an effective relative
permittivity, εr,e :
• The phase velocity and phase constant, respectively, are:
• In general,
• The upper bound occurs if the entire space above the microstrip has
the same permittivity as the substrate, while the lower bound
occurs if in this situation the material is chosen to be free space.
12
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
as for a typical TEM mode.
Microstrip lines….
• The characteristic impedance of the quasi-TEM mode on the microstrip
can be approximated as
13
ECE-601
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Lec#3
,
Nov
2014
©
Ahmad
El-Banna
• the attenuation
due to dielectric loss
• The attenuation due
to conductor loss
DESIGN OF MICROSTRIP LINES 14
ECE-601
,
Lec#3
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Nov
2014
©
Ahmad
El-Banna
Design Example
15
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
CAD tool
• Many tools are available for microwave CAD.
• The Rogers ACM Division introduces a new design program
that is free to download called the MWI-2010 Microwave
Impedance Calculator, a transmission line modeling tool for
electronics engineers.
• Link to download:
• http://www.rogerscorp.com/acm/technology/index.aspx
• Design the previous Example using the MWI-2010 Microwave
Impedance Calculator.
16
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
MULTI-LAYER MICROSTRIP LINES 17
ECE-601
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Lec#3
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Nov
2014
©
Ahmad
El-Banna
Ref: K. R. Jha and G. Singh, Terahertz Planar Antennas for Next Generation Communication, DOI:
10.1007/978-3-319-02341-0_2, Springer International Publishing Switzerland 2014
Multi-layer Microstrip lines
• In general, the microstrip line is used to conduct the
electromagnetic wave at low frequency.
• Beyond 60 GHz, its application is restricted due to the losses
in the line.
• Due to this, there is a general consideration that the use of
microstrip transmission line at THz frequency is impractical.
• Moving away from this theory, the microstrip transmission
line has successfully been used to transmit the THz wave.
• The transmission line parameters become frequency
dependent and need the empirical formula to evaluate these
parameters at such high frequency.
18
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
Necessity of Multilayer Microstrip
Transmission Line
• A microstrip transmission line can be designed on the different
configuration of the substrate layers which may be single, double, or
the multilayered material.
• With the development in the technology and the need of the
system-on-chip (SOC) requirement, the use of the multilayered
substrate has increased at high frequency.
• The use of the multilayered substrate material microstrip transmission
line has a numerous advantages such as:
• Capability to reduce the losses and to control the coefficient of
expansion.
• It is also an alternative solution to circuit layout and the combination of
the substrate and semiconductor layer gives the slow-wave structure.
• The multilayered substrate is also used in the antenna design where it
shows good surface wave immunity gain, and bandwidth
enhancement apart from the good mechanical integration. 19
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
20
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
The effective dielectric permittivity of the multilayered
substrate material is :
Characteristic Impedance
21
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
The dispersive behavior of characteristic
impedance on the multilayered substrate
material is obtained by
Effectof Substrate Layerson the
CharacteristicImpedance
22
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna
• For more details, refer to:
• Chapters 3, Microwave Engineering, David Pozar_4ed.
• Lecture Notes of , EE 481 - Microwave Engineering Course,
Laboratory for applied electromagnetic and communications,
South Dakota school for mines and technology, 2013.
• The lecture is available online at:
• http://bu.edu.eg/staff/ahmad.elbanna-courses/11983
• For inquires, send to:
• ahmad.elbanna@feng.bu.edu.eg
23
ECE-601
,
Lec#3
,
Nov
2014
©
Ahmad
El-Banna

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microstrip transmission lines explained.pdf

  • 1. Lecture #3 Microstrip lines Instructor: Dr. Ahmad El-Banna Benha University Faculty of Engineering at Shoubra November 2014 Post-Graduate ECE-601 Active Circuits © Ahmad El-Banna
  • 2. Agenda Striplines Forward & Reverse Striplines Design Microstrip lines Design of Microstrip lines Multi-layer Microstrip lines 2 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 4. Stripline Transmission Lines • Microwave circuits that supports TEM or “quasi-TEM” modes are: • Microstrip and covered microstrip • Stripline • Slotline • Coplanar waveguide. • Stripline has one or more interior strip conductors immersed in a dielectric with ground planes above and below. 4 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 5. Formulasfor PropagationConstant, CharacteristicImpedance,and Attenuation • Stripline can support the TEM mode exclusively provided that • At higher frequencies, TE and TM modes may also propagate, which leads to signal distortion and other undesirable effects. This is called an “over-moded” waveguide. • We’ll assume that the (carrier) frequency is “low” enough that and only the TEM mode propagates. As with any TEM mode, in a stripline with 5 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna none of these quantities depend on frequency for a TEM mode. propagation constant characteristic impedance of a transmission line phase velocity
  • 6. FORWARD & REVERSE STRIPLINES DESIGN 6 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 7. Forward Stripline Design • We will need to design stripline with a specific Z0. • Determining the C value is the problem. There is no simple, exact analytical solution for stripline (or microstrip, for that matter). • But extremely accurate numerical solutions can be found using a number of techniques including the method of moments and the finite element method, among others. • By curve fitting to these numerical solutions, it can be shown that for a stripline: 7 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna where We is called an “effective strip width” given by *These formulas assume a strip with zero thickness and are quoted as being accurate to about 1% of the exact results.
  • 8. Reverse Stripline Design • One can determine the “inverse” of Z0, so that W/ b can be determined once εr and the required Z0 are specified: • 8 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 10. Microstrip lines • One of the most widely used planar microwave circuit interconnections is microstrip. These are commonly formed by a strip conductor (land) on a dielectric substrate, which is backed by a ground plane. • We will often assume the land has zero thickness, t. • In practical circuits there will often be metallic walls and covers to protect the circuit. We will ignore these effects. • Unlike stripline, a microstrip has more than one dielectric in which the EM fields are located. • This presents a difficulty. 10 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 11. Microstrip lines.. • If the field propagates as a TEM wave, then • But which εr do we use? • The answer is neither because there is actually no purely TEM wave on the microstrip, but something that closely approximates it called a “quasi-TEM” mode. • At low frequency, this mode is almost exactly TEM. • Conversely, when the frequency becomes too high, there are axial components of E and/or H making the mode no longer quasi-TEM. • This property leads to dispersive behavior. • Numerical and other analysis have been performed on microstrip since approximately 1965. • Some techniques, such as the method of moments, produce very accurate numerical solutions to equations derived directly from Maxwell’s equations and incorporate the exact cross-sectional geometry and materials of the microstrip. 11 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 12. Microstrip lines… • From these solutions, simple and quite accurate analytical expressions for Z0, ʋp etc. have been developed primarily by curve fitting. • The result of these analyses is that at relatively “low” frequency, the wave propagates as a quasi-TEM mode with an effective relative permittivity, εr,e : • The phase velocity and phase constant, respectively, are: • In general, • The upper bound occurs if the entire space above the microstrip has the same permittivity as the substrate, while the lower bound occurs if in this situation the material is chosen to be free space. 12 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna as for a typical TEM mode.
  • 13. Microstrip lines…. • The characteristic impedance of the quasi-TEM mode on the microstrip can be approximated as 13 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna • the attenuation due to dielectric loss • The attenuation due to conductor loss
  • 14. DESIGN OF MICROSTRIP LINES 14 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 16. CAD tool • Many tools are available for microwave CAD. • The Rogers ACM Division introduces a new design program that is free to download called the MWI-2010 Microwave Impedance Calculator, a transmission line modeling tool for electronics engineers. • Link to download: • http://www.rogerscorp.com/acm/technology/index.aspx • Design the previous Example using the MWI-2010 Microwave Impedance Calculator. 16 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 17. MULTI-LAYER MICROSTRIP LINES 17 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna Ref: K. R. Jha and G. Singh, Terahertz Planar Antennas for Next Generation Communication, DOI: 10.1007/978-3-319-02341-0_2, Springer International Publishing Switzerland 2014
  • 18. Multi-layer Microstrip lines • In general, the microstrip line is used to conduct the electromagnetic wave at low frequency. • Beyond 60 GHz, its application is restricted due to the losses in the line. • Due to this, there is a general consideration that the use of microstrip transmission line at THz frequency is impractical. • Moving away from this theory, the microstrip transmission line has successfully been used to transmit the THz wave. • The transmission line parameters become frequency dependent and need the empirical formula to evaluate these parameters at such high frequency. 18 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 19. Necessity of Multilayer Microstrip Transmission Line • A microstrip transmission line can be designed on the different configuration of the substrate layers which may be single, double, or the multilayered material. • With the development in the technology and the need of the system-on-chip (SOC) requirement, the use of the multilayered substrate has increased at high frequency. • The use of the multilayered substrate material microstrip transmission line has a numerous advantages such as: • Capability to reduce the losses and to control the coefficient of expansion. • It is also an alternative solution to circuit layout and the combination of the substrate and semiconductor layer gives the slow-wave structure. • The multilayered substrate is also used in the antenna design where it shows good surface wave immunity gain, and bandwidth enhancement apart from the good mechanical integration. 19 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 20. 20 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna The effective dielectric permittivity of the multilayered substrate material is :
  • 21. Characteristic Impedance 21 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna The dispersive behavior of characteristic impedance on the multilayered substrate material is obtained by
  • 22. Effectof Substrate Layerson the CharacteristicImpedance 22 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna
  • 23. • For more details, refer to: • Chapters 3, Microwave Engineering, David Pozar_4ed. • Lecture Notes of , EE 481 - Microwave Engineering Course, Laboratory for applied electromagnetic and communications, South Dakota school for mines and technology, 2013. • The lecture is available online at: • http://bu.edu.eg/staff/ahmad.elbanna-courses/11983 • For inquires, send to: • ahmad.elbanna@feng.bu.edu.eg 23 ECE-601 , Lec#3 , Nov 2014 © Ahmad El-Banna