Rlc Basics

33
Chapter 13 RLC Circuits and Resonance

description

basics of rlc circuits

Transcript of Rlc Basics

Page 1: Rlc Basics

Chapter 13RLC Circuits and

Resonance

Page 2: Rlc Basics

Impedance of Series RLC

Circuits

• A series RLC circuit contains both inductance and

capacitance

• Since XL and XC have opposite effects on the

circuit phase angle, the total reactance (Xtot)is less

than either individual reactance

Page 3: Rlc Basics

Impedance of Series RLC

Circuits

• When XL>XC, the circuit is predominantly

inductive

• When XC> XL, the circuit is predominantly

capacitive

• Total reactance |XL – XC|

• Total impedance for a series RLC circuit is:

Ztot = √R2 + Xtot2

θ = tan-1(Xtot/R)

Page 4: Rlc Basics

Analysis of Series RLC Circuits

• A series RLC circuit is:

• Capacitive when XC>XL

• Inductive when XL>XC

• Resonant when XC=XL

• At resonance Ztot = R

• XL is a straight line

y = mx + b

• XC is a hyperbola

xy = k

Page 5: Rlc Basics

Series RLC impedance as a function of frequency.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Graph Including Ztot = R at Resonance

Page 6: Rlc Basics

Voltage Across the Series

Combination of L and C

• In a series RLC circuit, the capacitor

voltage and the inductor voltage are always

180° out of phase with each other

• Because they are 180° out of phase, VC and

VL subtract from each other

• The voltage across L and C combined is

always less that the larger individual

voltage across either element

Page 7: Rlc Basics

The voltage across the series combination of C and L is always less than the larger individual voltage across

either C or L

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 8: Rlc Basics

Inductor voltage and capacitor voltage effectively subtract because they are out of phase

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 9: Rlc Basics

Series Resonance

• Resonance is a condition in a series RLC

circuit in which the capacitive and inductive

reactances are equal in magnitude

• The result is a purely resistive impedance

• The formula for series resonance is:

LCπ2

1

Page 10: Rlc Basics

At the resonant frequency (fr), the reactances are equal in magnitude and effectively cancel, leaving Zr = R

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Xtot = 0

Page 11: Rlc Basics

•At the resonant frequency, fr, the voltages across C and L are equal in magnitude.

Since they are 180º out of phase with each other, they cancel, leaving 0 V across the CL

combination (point A to point B).

The section of the circuit from A to B effectively looks like a short at resonance

(neglecting winding resistance).

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 12: Rlc Basics

An illustration of how the voltage and current amplitudes respond in a series RLC circuit as the frequency is

increased from below to above its resonant value. The source voltage is held at a constant amplitude

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Frequency below Resonance

Xc > XL

Frequency at Resonance

Xc = XL

Frequency above Resonance

Xc < XL

Page 13: Rlc Basics

Generalized current and voltage magnitudes as a function of frequency in a series RLC circuit. VC and VL can be

much larger than the source voltage. The shapes of the graphs depend on particular circuit values.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 14: Rlc Basics

Phase Angle of a Series RLC

Circuit

Capacitive = ICE Inductive = ELI

Page 15: Rlc Basics

A basic series resonant band-pass filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 16: Rlc Basics

Bandwidth of Series Resonant

Circuits• Current is maximum at

resonant frequency

• Bandwidth (BW) is the

range between two cutoff

frequencies (f1 to f2)

• Within the bandwidth

frequencies, the current is

greater than 70.7% of the

highest resonant value

Page 17: Rlc Basics

FIGURE 13-22 Generalized selectivity curve of a band-pass filter.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

The 70.7% cutoff point is also referred to as:

•The Half Power Point

•-3dB Point

AKA:

•Half Power

•-3dB

Page 18: Rlc Basics

Formula for Bandwidth

• Bandwidth for either series or parallel

resonant circuits is the range of frequencies

between the upper and lower cutoff

frequencies for which the response curve (I

or Z) is 0.707 of the maximum value

BW = f2 - f1

• Ideally the center frequency is:

fr = (f1 + f2)/2

Page 19: Rlc Basics

Example of the frequency response of a series resonant band-pass filter with the input voltage at a

constant 10 V rms. The winding resistance of the coil is neglected.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 20: Rlc Basics

Selectivity

• Selectivity defines how well a resonant circuit responds to a certain frequency and discriminates against all other frequencies

• The narrower the bandwidth steeper the slope, the greater the selectivity

• This is related to the Quality (Q) Factor (performance) of the inductor at resonance. A higher Q Factor produces a tighter bandwidth– Q = X L/(R + Rwindings)

– Bandwidth = Fr/Q

Page 21: Rlc Basics

FIGURE 13-23 Comparative selectivity curves.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 22: Rlc Basics

A basic series resonant band-stop filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 23: Rlc Basics

Generalized response curve for a band-stop filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 24: Rlc Basics

Example of the frequency response of a series resonant band-stop filter with Vin at a constant 10 V rms. The

winding resistance is neglected.

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 25: Rlc Basics

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Parallel RLC Circuits - Skip

Page 26: Rlc Basics

Tank Circuit

• A parallel resonant circuit stores energy in the

magnetic field of the coil and the electric field of

the capacitor. The energy is transferred back and

forth between the coil and capacitor

Page 27: Rlc Basics

Parallel Resonant Circuits

• For parallel resonant circuits, the impedance is maximum (in theory, infinite) at the resonant frequency

• Total current is minimum at the resonant frequency

• Bandwidth is the same as for the series resonant circuit; the critical frequency impedances are at 0.707Zmax

Page 28: Rlc Basics

A basic parallel resonant band-pass filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 29: Rlc Basics

Generalized frequency response curves for a parallel resonant band-pass filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

AKA:

•Half Power

•-3dB

Page 30: Rlc Basics

Example of the response of a parallel resonant band-pass filter with the input voltage at a constant 10 V rms

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 31: Rlc Basics

A basic parallel resonant band-stop filter

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 32: Rlc Basics

A simplified portion of a TV receiver showing filter usage

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Passing Audio Frequency Carrier (4.5 MHz)

Blocking Audio Frequency Carrier (4.5 MHz)

Page 33: Rlc Basics

A simplified diagram of a superheterodyne AM radio broadcast receiver showing the application of tuned resonant circuits

Thomas L. Floyd

Electronics Fundamentals, 6e

Electric Circuit Fundamentals, 6e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Intermediate Frequency (IF) is:

Local oscillator frequency

- Carrier Frequency

1055Khz

- 600 Khz

455 KhzTank Circuits used as Oscillators

455 Khz

Bandpass

Filter

Local Oscillator is

always 455 Khz above

Tuner Frequency

600 Khz

Bandpass

Filter

600 Khz

Tuned Frequency