5. rc and rl first-order circuits

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5. RC AND RL FIRST-ORDER CIRCUITS CIRCUITS by Ulaby & Maharbiz

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5. RC and RL First-Order Circuits. CIRCUITS by Ulaby & Maharbiz. Overview. Transient Response. Non-Periodic Waveforms. Step Function. Ramp Function. Square Pulse. Exponential. Non-Periodic Waveforms: Step Function. Non-Periodic Waveforms: Ramp Function. - PowerPoint PPT Presentation

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Page 1: 5. RC and RL First-Order Circuits

5. RC AND RL FIRST-ORDER CIRCUITS

CIRCUITS by Ulaby & Maharbiz

Page 2: 5. RC and RL First-Order Circuits

Overview

Page 3: 5. RC and RL First-Order Circuits

Transient Response

Page 4: 5. RC and RL First-Order Circuits

Non-Periodic WaveformsStep

Function

Square Pulse

Ramp Function

Exponential

Page 5: 5. RC and RL First-Order Circuits

Non-Periodic Waveforms: Step Function

Page 6: 5. RC and RL First-Order Circuits

Non-Periodic Waveforms: Ramp Function

Page 7: 5. RC and RL First-Order Circuits

Waveform synthesis as sum of two ramp functions

Page 8: 5. RC and RL First-Order Circuits

Non-Periodic Waveforms: Pulses

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Waveform Synthesis1. Pulse 2. Trapezoid

Page 10: 5. RC and RL First-Order Circuits

Non-Periodic Waveforms: Exponentials

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Page 12: 5. RC and RL First-Order Circuits

CapacitorsPassive element that stores energy in

electric fieldParallel plate capacitor

dAC

0o

1 tdtiC

t

t

For DC, capacitor looks like open circuit

Voltage on capacitor must be continuous (no abrupt change)

Page 13: 5. RC and RL First-Order Circuits

Various types of capacitors

Page 14: 5. RC and RL First-Order Circuits

Capacitors in Fingerprint Imager

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Tech Brief 11: Supercapacitors

A new generation of capacitor technologies, termed supercapacitors or ultracapacitors, is narrowing the gap between capacitors and batteries. These capacitors can have sufficiently high energy densities to approach within 10 percent of battery storage densities, and additional improvements may increase this even more. Importantly, supercapacitors can absorb or release energy much faster than a chemical battery of identical volume. This helps immensely during recharging. Moreover, most batteries can be recharged only a few hundred times before they are degraded completely; supercapacitors can be charged and discharged millions of times before they wear out. Supercapacitors also have a much smaller environmental footprint than conventional chemical batteries, making them particularly attractive for green energy solutions.

Page 16: 5. RC and RL First-Order Circuits

Energy Stored in Capacitor

Page 17: 5. RC and RL First-Order Circuits

Capacitor Response: Given v(t), determine i(t), p(t), and w(t)

C =

Page 18: 5. RC and RL First-Order Circuits

RC Circuits at dc At dc no currents flow through capacitors: open circuits

Page 19: 5. RC and RL First-Order Circuits

Capacitors in SeriesUse KVL, current

same through each capacitor

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Capacitors in Parallel

NCCCCC 321eq

Use KCL, voltage same across each

capacitor

Page 21: 5. RC and RL First-Order Circuits

Voltage Division

Page 22: 5. RC and RL First-Order Circuits

InductorsPassive element that stores energy in

magnetic field

0o

1 tidttvL

it

t

At dc, inductor looks like a short circuit

Current through inductor must be continuous (no abrupt change)

lANL 2

Solenoid Wound Inductor

Page 23: 5. RC and RL First-Order Circuits

Inductor Response to

Page 24: 5. RC and RL First-Order Circuits

Inductors in SeriesUse KVL, current is same through all

inductors

Page 25: 5. RC and RL First-Order Circuits

Inductors in Parallel

Voltage is same across all inductors

Inductors add together in the same

way resistors do

Page 26: 5. RC and RL First-Order Circuits

RL Circuits at dc At dc no voltage across inductors: short circuit

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Page 28: 5. RC and RL First-Order Circuits

Response Terminology

Natural response – response in absence of sourcesForced response – response due to external source

Complete response = Natural + Forced

Transient response – time-varying response (temporary)Steady state response – time-independent or periodic (permanent)

Complete response = Transient + Steady State

Source dependence

Time dependence

Page 29: 5. RC and RL First-Order Circuits

Natural Response of Charged Capacitor

(a) t = 0− is the instant just before the switch is moved from terminal 1 to terminal 2

(b) t = 0 is the instant just after it was moved;

t = 0 is synonymous with t = 0+since the voltage across the capacitor cannot change instantaneously, it follows that

Page 30: 5. RC and RL First-Order Circuits

Solution of First-Order Diff. Equations

τ is called the time constant of the circuit.

Page 31: 5. RC and RL First-Order Circuits

Natural Response of Charged Capacitor

Page 32: 5. RC and RL First-Order Circuits

General Response of RC Circuit

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Solution of

Page 34: 5. RC and RL First-Order Circuits

Example 5-9: Determine Capacitor Voltage

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Example 5-9 Solution

At t = 0

At t > 0

(a) Switch was moved at t = 0

(b) Switch was moved at t = 3 s

Page 36: 5. RC and RL First-Order Circuits

Example 5-10: Charge/Discharge Action

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Example 5-10 (cont.)

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Example 5-11: Rectangular Pulse

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Natural Response of the RL Circuit

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General Response of the RL Circuit

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Example 5-12: Two RL Branches

At t=0-

Cont.

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Example 5-12: Two RL Branches (cont.)

After t=0:

Page 43: 5. RC and RL First-Order Circuits

RC Op-Amp Circuits: Ideal Integrator

Page 44: 5. RC and RL First-Order Circuits

Example 5-14: Square-Wave Signal

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RC Op-Amp Circuits: Ideal Differentiator

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Example 5-15: Pulse Response

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Multisim Example

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Summary