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Lecture 12 Smith Chart & VSWR. 6.013. ELECTROMAGNETICS AND APPLICATIONS. Luca Daniel. Examples of Z(z) transformations. Example: Open Circuit Load, Z L = :. capacitor C o. 0 when z = - /4, -3/4,…. z. short circuit every half wavelength. z =- D. 0. Short circuit. Open circuit.
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Lecture 12Smith Chart & VSWR 6.013 ELECTROMAGNETICS AND APPLICATIONS Luca Daniel
Examples of Z(z) transformations Example: Open Circuit Load, ZL = : capacitor Co • 0 when z = -/4, -3/4,… z short circuit every half wavelength z =-D 0 Short circuit Open circuit Im{Z} when z = 0, -/2,… open circuit every half wavelength z 0 - In general: -j < Z(-D) < +j (can get ANY desired capacitance or inductance at a SINGLE w)
L Zo ? o z l/4 0 Examples of Z(z) transformations (cont) Example: half-wave and quarter-wave lines: Zo ZL ? z 0 Example: quarter-wave with inductive load:
(5) (4) (3) (1) (2) Alternative approach to finding Z(z) I(z) Normalize Load: + ZL Zo,n V(z) - z Compute reflection coef: z = - D 0 Z(z) or “find” it on the plane (Smith Chart) Im{} “Rotate” reflection coef. Im{Zn}=+j inductor = j (toward generator clockwise) (D= /2 full rotation) Re{Zn}=3 Re{Zn} = 0 Re{Zn}=1 Im{Zn}=0 resistor Compute Normalized Line Impedance = 1 = -1 Re{} = 0 Zn = open Zn = 1 Z =Z0 Zn = 0 short or “read” it from Smith Chart Im{Zn} = -j capacitor “Un-Normalize” Line Impedance toward z=-D = -j
Voltage Standing Wave Ratio (VSWR) + ZL Zo,n V(z) - z Im{} 0 toward z=-D Re{} -1 z 0 -D