AC Circuits

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In this chapter, we will study the circuits with the steady-state ... reached. This is referred to as steady-state AC analysis. AC Circuits 4 ... numbers. AC Circuits 8.
PHYS 3050 – Electronics I Chapter 2. AC Circuits

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Dr. Jinjun Shan, Associate Professor of Space Engineering Department of Earth and Space Science and Engineering Room 255, Petrie Science and Engineering Building Tel: 416-736 2100 ext. 33854 Email: [email protected] Homepage: http://www.yorku.ca/jjshan

Introduction 







For DC circuits, we can have steady voltages and currents. In this chapter, we will study the circuits with the steady-state analysis of AC circuits. The simplest and occur widely timevarying voltages and currents are sinusoidal. Special characteristic of sinusoids AC Circuits 2

Introduction

If a linear circuit is driven by a sinusoidal source, then all responses anywhere in the circuit are also sinusoidal. This applies only after all initial transients have died down and a steady-state is reached. This is referred to as steady-state AC analysis. AC Circuits 3

Sinusoidal Driving Functions

If the voltage or current source is sinusoidal, all voltages and currents anywhere in the linear circuit will also be sinusoidal.

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Sinusoidal Driving Functions

Out of phase

In phase

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Phasor Analysis

Phasor:

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Basis of Phasor Analysis

1) First, we recognize that we are dealing with a linear circuit. 2) The circuit equation is basically a linear differential equation (LDE) with constant coefficients. 3) Natural solutions to LDEs with constant coefficients are exponentials. All calculations will be in terms of complex numbers.

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Basis of Phasor Analysis

4) Let the real source be given by Vpcosωt=ReVp·exp(jωt) 5) The solution for the current I·exp(jωt), phasor I. 6) Convert phasor I to real-time current i(t) by simply multiplying I by exp(jωt) and take the real part, i.e. i(t) = ReI·exp(jωt). AC Circuits 8

Basis of Phasor Analysis

Example: Change the voltage source in RLC circuit to v(t) = Vpcos(ωt+ϕ), find current i(t) in the circuit.

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Impedance and Phasor Relationship

 For AC circuits, Ohm’s law becomes V=IZ, where Z is a complex number.  We can generalize and state that AC circuit analysis is DC analysis with complex numbers.  This is a powerful statement and means that all the circuit laws that were derived previously apply equally to AC circuits. AC Circuits 10

Impedance and Phasor Relationship

Example: Find voltage V2 in this figure when it is driven by V = cos2t.

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Admittance

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High-Pass and Low-Pass Filters 

RC Filters

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High-Pass and Low-Pass Filters 

High-Pass RC Filter

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High-Pass and Low-Pass Filters 

RL Filters

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High-Pass and Low-Pass Filters 

High-Pass RL Filter

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Resonance and Band-Pass Filters 

With RC and RL, we can have low-pass or high-pass filters. If we add both energy-storing elements to resistor, we can obtain band-pass or band-rejection action.



Band-pass filters can be used as tuning circuits where they allow one station or more channel out of many to be selected. AC Circuits 17

Resonance and Band-Pass Filters 

Series Resonance

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Resonance and Band-Pass Filters 

Notch Filter

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Resonance and Band-Pass Filters 

Parallel Resonance

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Resonance and Band-Pass Filters 

Q-Factor and Bandwidth

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Power in AC and RF Circuits 

Reading: Section 2.5

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Transformers and Impedance Matching 

Reading: Section 2.6

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