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CIRCUITS by Ulaby & Maharbiz
7. AC Analysis CIRCUITS by Ulaby & Maharbiz
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Overview
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Linear Circuits at ac Objective: To determine the steady state response of a linear circuit to ac signals Sinusoidal input is common in electronic circuits Any time-varying periodic signal can be represented by a series of sinusoids (Fourier Series) Time-domain solution method can be cumbersome
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Sinusoidal Signals Useful relations
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Phase Lead/Lag
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Complex Numbers We will find it is useful to represent sinusoids as complex numbers Rectangular coordinates Polar coordinates Relations based on Euler’s Identity
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Relations for Complex Numbers
Learn how to perform these with your calculator/computer
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Phasor Domain 1. The phasor-analysis technique transforms equations
from the time domain to the phasor domain. 2. Integro-differential equations get converted into linear equations with no sinusoidal functions. 3. After solving for the desired variable--such as a particular voltage or current-- in the phasor domain, conversion back to the time domain provides the same solution that would have been obtained had the original integro-differential equations been solved entirely in the time domain.
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Phasor Domain Phasor counterpart of
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Time and Phasor Domain It is much easier to deal with exponentials in the phasor domain than sinusoidal relations in the time domain. You just need to track magnitude/phase, knowing that everything is at frequency w.
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Phasor Relation for Resistors
Current through a resistor Time domain Time Domain Frequency Domain Phasor Domain
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Phasor Relation for Inductors
Current through inductor in time domain Time domain Phasor Domain Time Domain
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Phasor Relation for Capacitors
Voltage across capacitor in time domain is Time domain Time Domain Phasor Domain
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Summary of R, L, C
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ac Phasor Analysis General Procedure
Using this procedure, we can apply our techniques from dc analysis
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Example 1-4: RL Circuit Cont.
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Example 1-4: RL Circuit cont.
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Impedance and Admittance
Impedance is voltage/current Admittance is current/voltage R = resistance = Re(Z) G = conductance = Re(Y) X = reactance = Im(Z) B = susceptance = Im(Y) Resistor Inductor Capacitor
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Impedance Transformation
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Voltage & Current Division
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Cont.
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Example 7-6: Input Impedance (cont.)
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Example 7-9: Thévenin Circuit
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Linear Circuit Properties
Thévenin/Norton and Source Transformation Also Valid
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Phasor Diagrams
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Phase-Shift Circuits
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Example 7-11: Cascaded Phase Shifter
Solution leads to:
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Node 1 Cont.
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(cont.) Cont.
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(cont.)
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Example 7-14: Mesh Analysis by Inspection
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Example 7-16: Thévenin Approach
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Example 7-16: Thévenin Approach (Cont.)
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Example 7-16: Thévenin Approach (Cont.)
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Power Supply Circuit
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Ideal Transformer
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Half-Wave Rectifier
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Full-Wave Rectifier Current flow during first half of cycle
Current flow during second half of cycle
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Smoothing RC Filter
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Complete Power Supply
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Example 7-20: Multisim Measurement of Phase Shift
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Example 7-20 (cont.) Using Transient Analysis
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Summary
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