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Objective of Lecture Describe the mathematical relationships between ac voltage and ac current for a resistor, capacitor, and inductor. Discuss the phase relationship between the ac voltage and current. Chapter 9.4 Fundamentals of Electric Circuits Explain how Ohm’s Law can be adapted for inductors and capacitors when an ac signal is applied to these components. Derive the mathematical formulas for the impedance and admittance of a resistor, inductor, and capacitor. Chapter 9.5 Fundamentals of Electric Circuits Resistors Ohm’s Law if i(t) = Im cos(wt + q) then v(t) = Ri(t) = R Im cos(wt + q) V = RIm q = RI where q = f The voltage and current through a resistor are in phase as there is no change in the phase angle between them. Capacitors i(t) = C dv(t)/dt where v(t) = Vm cos(wt) i(t) = -Cw Vm sin(wt) i(t) = wCVm sin(wt + 180o) i(t) = wCVm cos(wt + 180o - 90o) i(t) = wCVm cos(wt + 90o) Capacitors V = Vm0o I = wCVm cos(wt + 90o) Vm cos(wt + 90o) = V ej90 = V90o = jV I = jwCV = wCV90o or V = (1/jwC) I = - (j/wC) I = (1/wC) I-90o Capacitors 90o phase difference between the voltage and current through a capacitor. Current needs to flow first to place charge on the electrodes of a capacitor, which then induce a voltage across the capacitor Current leads the voltage (or the voltage lags the current) in a capacitor. Inductors v(t) = L d i(t)/dt where i(t) = Im cos(wt) v(t) = - Lw Im sin(wt) = wLIm cos(wt + 90o) V = wLIm 90o I = Im cos(wt) Im cos(wt + 90o) = I ej90 = I 90o = jI V = jwLI = wLI90o or I = (1/jwL) V = - (j/wL) V = (1/wL) V-90o Inductors 90o phase difference between the voltage and current through an inductor. The voltage leads the current (or the current lags the voltage). Impedance If we try to force all components to following Ohm’s Law, V = Z I, where Z is the impedance of the component. Resistor: Capacitor: Inductor: ZR = R ZC = j wC ZL = jwL R0o 1 wC 90o wL90o Admittance If we rewrite Ohm’s Law: I = Y V (Y = 1/Z), where Y is admittance of the component o 1 / R = G G 0 Resistor: YR = wC90o Capacitor: YC = jwC Inductor: YL = j wL 1 wL 90o Impedances Value at w = Admittance s 0 rad/s ∞ rad/s Value at w = 0 rad/s ∞ rad/s ZR = R = 1/G R R YR = 1/R = G G G ZL = jwL 0W ∞W YL =-j/(wL) ∞ W1 0 W1 ZC = -j/(wC) ∞W 0W YC = jwC 0 W1 ∞ W1 Inductors act like short circuits under d.c. conditions and like open circuits at very high frequencies. Capacitors act like open circuits under d.c. conditions and like short circuits at very high frequencies. Impedance Generic component that represents a resistor, inductor, or capacitor. Z = Z f Z = R + jX Z = R +X 2 f = tan 1 2 X R R = Z cos f X = Z sin f Admittance 1 Y =1 Z = R + jX R G= 2 R +X2 X B= 2 R +X2 Y = Y Y = G + jB Y = G2 + B2 = tan 1 B G G = Y cos B = Y sin Summary Ohm’s Law can be used to determine the ac voltages and currents in a circuit when impedance or admittance are used. A resistor’s voltage and current are in phase. Voltage leads current through an inductor by 90o. Current leads voltage through a capacitor by 90o. Component Impedance Resistor ZR Capacitor ZC Inductor ZL R Admittance R 0o j wC 1 wC 90o jwL wL + 90 G jwC G 0o wC + 90 j wL 1 wL 90o