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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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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.
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
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
e Z
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 up Example: 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,