Transmission Lines: Wavelength, Propagation Mode, and Equations in ECE 1266 - Prof. Joel F, Study notes of Electrical and Electronics Engineering

Course notes for the ece 1266 applications of fields and waves class, focusing on transmission lines, their wavelength, propagation modes, and the lumped-element model. The notes cover the concepts of t-lines, tem waves, and the telegrapher's equations. Students will learn when to consider a line as a t-line, the lumped-element model, and the telegrapher's equations in both frequency and time domains.

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Course Notes for ECE 1266 Applications of fields and waves
NOTES for Transmission Lines I
This lecture covers Chapter 6.1 and 6.2
1. Transmission lines (T-lines), wavelength,
propagation mode
2. Lumped-element model
3. Telegrapher’s equation and solution
1. Transmission lines, wavelength, and TEM wave
Transmission lines are used as a carrier to transmit
transverse EM waves. A T-line connects generator circuits
to loads. A transverse EM (TEM) wave is a special EM
wave, which will be defined below.
When do we need to consider a “line” to be T-line? When
the wavelength of TEM waves is comparable or smaller
than the length of “the line”, we will need to consider the
“line” a T-line. Just give a few rough examples
oA coaxial cable of 1 m length is just a wire if it
transmits signal with frequency of 1 MHz. Because the
wavelength of the TEM wave at this frequency is c/f~
100-300 meter (the speed of the light on the coaxial
cable is smaller than 3 108 meter/s). However when the
signal has frequency of 1 GHz, “this line” becomes a
T-line because the wavelength of the EM wave is <0.3
meter, and therefore the voltage along the line varies
along “the line”.
oConducting wires on a CPU chip can be a few
meters long. They are just “a line” when clock
frequency is ~10 MHz (20 years ago). They must be
considered T-lines today because the CPU runs at a 2-
3 GHz clock frequency.
Below are some examples of T-lines. Not all of the lines
can be considered as T-lines. Strictly speaking, only
structures that support TEM waves can be considered T-
lines. Because the E-field starts from one conducting plate
and ends at the other one, which means the voltages
Chapter 6: Lecture 1 1
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NOTES for Transmission Lines I

This lecture covers Chapter 6.1 and 6.

1. Transmission lines (T-lines), wavelength,

propagation mode

2. Lumped-element model

3. Telegrapher’s equation and solution

1. Transmission lines, wavelength, and TEM wave

 Transmission lines are used as a carrier to transmit transverse EM waves. A T-line connects generator circuits to loads. A transverse EM (TEM) wave is a special EM wave, which will be defined below.  When do we need to consider a “line” to be T-line? When the wavelength of TEM waves is comparable or smaller than the length of “the line”, we will need to consider the “line” a T-line. Just give a few rough examples o A coaxial cable of 1 m length is just a wire if it transmits signal with frequency of 1 MHz. Because the wavelength of the TEM wave at this frequency is c/f~ 100-300 meter (the speed of the light on the coaxial cable is smaller than 3 10^8 meter/s). However when the signal has frequency of 1 GHz, “this line” becomes a T-line because the wavelength of the EM wave is <0. meter, and therefore the voltage along the line varies along “the line”. o Conducting wires on a CPU chip can be a few meters long. They are just “a line” when clock frequency is ~10 MHz (20 years ago). They must be considered T-lines today because the CPU runs at a 2- 3 GHz clock frequency.  Below are some examples of T-lines. Not all of the lines can be considered as T-lines. Strictly speaking, only structures that support TEM waves can be considered T- lines. Because the E-field starts from one conducting plate and ends at the other one, which means the voltages

between two conducting plates are well-defined, we can use a lumped-element model to describe the structures below in terms of R. L and C circuits.

2. Lumped-element model

Because we have a well-defined voltage between two conducting plates, we can use a pair of wires to represent any T-line structures. The voltage is measured between the lines and currents flow on both lines shown in the figure below. Along the length of any T-line structure, EM waves will incur loss and phase changes. This change depends on the frequency of EM waves. All these can effects be well described by R L C circuits. It is not hard to imagine that the R L and C along the T-lines depend linearly on the length of the T-lines. This means that distributed parameters will be needed to describe voltage and current along the transmission line:  R’ : The combined resistance of both conductors per unit length (/m)  L’ : The combined inductance of both conductors per unit length (H/m)  G’ : The conductance of the insulation medium per unit length (S/m)  C’ : The capacitance of the two conductors per unit length (F/m) It can be proven that for all TEM T-lines, the following relationships hold:      ' ' ' ' C G L C If the insulating medium between the conductors is air, the transmission line is called an air line. For an air line  =0 ,=0 ,=0, and G’= Example: Provide a lumped-element model for the co-axial cable shown below.

To solve the telegrapher’s equation, we take derivative of the first equation respect to z , then substitute the 2nd^ equation into the first. We get

2 2 2 2 2 2 j R j L G j C I z dz d I z V z dz dV z     

The parameter  is called a complex propagation constant,  is an attenuation constant (Np/m), and  as phase (propagation) constant (rad/m). The equations for V(z) and I(z) can be easily solved. z z z z I z I e I e V z V e V e               0 0 0 0 ( ) ( ) Both V(z) and I(z) contain two terms, the forward propagation wave (1st^ term) and the backward term (2nd^ term). Now, we have four variables,  V 0 (^) ,  V 0 (^) ,  I (^) 0 and  I (^) 0. We can reduce the number of variable to two by observing the relationship between voltage and current waves. We first substitute V(z) into the voltage telegrapher equation. We have

 V e z^ V ez  I e z I ez

R j L I z^ ^ ^ ^    (^)            (^0000) ' ' ( ) We compare two exponential terms and find:             0 0 0 0 0 ' ' ' ' ' ' I V I V G j C R j L R j L Z     The parameter Z 0 is a very important parameter. It is called the characteristics impedance of the transmission line. With the definition of the Z 0 , we now re-write the solutions for current and voltage: z z z z e Z

V

e Z

V

I z V z V e V e     0 0 0 0 0 0 ( )

       

The solution represents a forward propagating and a backward propagating solution. In general, the constant γ is complex and can be written in terms of its real and imaginary parts γ = α+jβ. The jβ. The propagation phase velocity is determined from β   upExample: A air T-line is a T-line for which air is the dielectric material present between the two metal wires, which renders G’=0. If the conductors are super good so R=0. If this T-line has a characteristics Z 0 =50 , and the phase constant =20 rad/m at 700 MHz. Find L’ and C’. File updated: September 12, 2006, minor change September 25,

  1. File updated September 12, 2007.