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Advanced Microwave Measurements
ECE 451 Advanced Microwave Measurements Transmission Lines Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois
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Maxwell’s Equations Faraday’s Law of Induction Ampère’s Law
Gauss’ Law for electric field Gauss’ Law for magnetic field Constitutive Relations
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Why Transmission Line? Wavelength : l propagation velocity l =
z Wavelength : l propagation velocity l = frequency
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Why Transmission Line? In Free Space At 10 KHz : l = 30 km At 10 GHz :
= 3 cm Transmission line behavior is prevalent when the structural dimensions of the circuits are comparable to the wavelength.
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Justification for Transmission Line
Let d be the largest dimension of a circuit circuit z l If d << l, a lumped model for the circuit can be used
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Justification for Transmission Line
circuit z l If d ≈ l, or d > l then use transmission line model
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Telegraphers’ Equations
L: Inductance per unit length. C: Capacitance per unit length. Assume time-harmonic dependence
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TL Solutions
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TL Solutions (Frequency Domain) forward wave backward wave
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TL Solutions Propagation constant Propagation velocity Wavelength
Characteristic impedance
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Reflection Coefficient
At z=0, we have V(0)=ZRI(0) But from the TL equations: Which gives where is the load reflection coefficient
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Reflection Coefficient
- If ZR = Zo, GR=0, no reflection, the line is matched - If ZR = 0, short circuit at the load, GR=-1 - If ZR inf, open circuit at the load, GR=+1 V and I can be written in terms of GR
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Impedance transformation equation
Generalized Impedance Impedance transformation equation
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Generalized Impedance
- Short circuit ZR=0, line appears inductive for 0 < l < l/2 - Open circuit ZR inf, line appears capacitive for 0 < l < l/2 - If l = l/4, the line is a quarter-wave transformer
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Generalized Reflection Coefficient
transformation equation
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Voltage Standing Wave Ratio (VSWR)
We follow the magnitude of the voltage along the TL Maximum and minimum magnitudes given by
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Voltage Standing Wave Ratio (VSWR)
Define Voltage Standing Wave Ratio as: It is a measure of the interaction between forward and backward waves
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VSWR – Arbitrary Load Shows variation of amplitude along line
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VSWR – For Short Circuit Load
Voltage minimum is reached at load
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VSWR – For Open Circuit Load
Voltage maximum is reached at load
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VSWR – For Open Matched Load
No variation in amplitude along line
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Application: Slotted-Line Measurement
Measure VSWR = Vmax/Vmin Measure location of first minimum
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Application: Slotted-Line Measurement
At minimum, Therefore, So, Since then and
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Summary of TL Equations
Voltage Current Impedance Transformation Reflection Coefficient Transformation Reflection Coefficient – to Impedance Impedance to Reflection Coefficient
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Example 1 Consider the transmission line system shown in the figure above. (a) Find the input impedance Zin.
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Example 1 – Cont’ (b) Find the current drawn from the generator
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Example 1 – Cont’ c) Find the time-average power delivered to the load
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Example 1 – Cont’ In the system shown above, a line of characteristic impedance 50 W is terminated by a series R, L, C circuit having the values R = 50 W, L = 1 mH, and C = 100 pF. (d) Find the source frequency fo for which there are no standing waves on the line.
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Example 1 – Cont’ No standing wave on the line if ZR = R = Zo which occurs at the resonant frequency of the RLC circuit. Thus,
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