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RLC Circuits Ohm for AC An AC circuit is made up with V0 sin t VR IR R VC IX C C X C 1 C • • • • Power source Resistors Capacitor Inductors Kirchhoff’s laws apply just like DC. • Special case for phase VL IX L L components. X L L Series RLC A series RLC circuit can be made from each component. i R v L • One loop • Same current everywhere Reactances are used for the capacitors and inductors. C The combination of resistances and reactances in a circuit is called impedance. Vector Map Phase shifts are present in AC circuits. • +90° for inductors • -90° for capacitors VL=IXL VR=IR These can be treated as if on the y-axis. • 2 D vector • Phasor diagram VC=IXC Vector Sum The current is the same in the loop. • Phasor diagram for impedance A vector sum gives the total impedance. XL XC XL Z R R XC Vector Sum The total impedance is the magnitude of Z. XC XL Z f The phase between the current and voltage is the angle f between Z and the x-axis. R Z R2 X L X C 2 1 2 Z R L C 2 X L XC tan f R 1 L C f arctan R Phase Changes The phase shift is different in each component. Power Factor Power loss in an AC circuit depends on the instantaneous voltage and current. • Applies to impedance p vi i 2 Z cos f The cosine of the phase angle is the power factor. 2 Prms Vrms I rms I rms Z cos f P I 0 Z cos f 2 0 t next