chapter 14: rlc circuits and resonance

14
Learning with Purpose Slide 1 Learning with Purpose Slide 1 Chapter 14: RLC Circuits and Resonance Instructor: Jean-Franรงois MILLITHALER http://faculty.uml.edu/JeanFrancois_Millithaler/FunElec/Spring2017

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Page 1: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 1

Learning with PurposeSlide 1

Chapter 14: RLC Circuits and Resonance

Instructor: Jean-Franรงois MILLITHALER

http://faculty.uml.edu/JeanFrancois_Millithaler/FunElec/Spring2017

Page 2: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 2

๐‘‹๐ฟ = 2๐œ‹๐‘“๐ฟ

๐‘‹๐ถ =1

2๐œ‹๐‘“๐ถ

IMPEDANCE AND PHASE ANGLE OF SERIES RLC CIRCUITS

๐‘tot = ๐‘๐‘… + ๐‘๐ฟ + ๐‘๐ถ

๐‘tot = ๐‘… + ๐‘—๐œ”๐ฟ +1

๐‘—๐œ”๐ถ

๐‘tot = ๐‘… + ๐‘— ๐œ”๐ฟ โˆ’1

๐œ”๐ถ

๐‘tot = ๐‘…2 + ๐œ”๐ฟ โˆ’1

๐œ”๐ถ

2

๐œƒ = ๐‘ก๐‘Ž๐‘›โˆ’1๐œ”๐ฟ โˆ’

1๐œ”๐ถ

๐‘…

Page 3: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 3

In a series RLC circuit, the circuit can be capacitive or inductive, depending on the frequency.

At the frequency where ๐‘ฟ๐‘ช = ๐‘ฟ๐‘ณ, the circuit is at series resonance.

Below the resonant frequency, the circuit is predominantly capacitive.

Above the resonant frequency, the circuit is predominantly inductive.

Variation of ๐‘ฟ๐‘ณ and ๐‘ฟ๐‘ช with frequency

Page 4: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 4

Exercice

Page 5: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 5

Example

Page 6: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 6

The voltages across the RLC components must add to the source voltage in accordance with KVL. Because of the opposite phase shift due to L and C, VL and VC effectively subtract.

Notice that VC is out of phase with VL. When they are algebraically added, the result isโ€ฆ

Voltages in a series RLC circuits

Page 7: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 7

Exercice

Page 8: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 8

At series resonance, XC and XL cancel. VC and VL also cancel because the voltages are equal and opposite. The circuit is purely resistive at resonance.

Series Resonance

Page 9: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 9

Series Resonance

At the resonant frequency, ๐‘“๐‘Ÿ, the voltages across C and L are equal in magnitude.

Since they are 180๐‘œ 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).

Page 10: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 10

For a given series RLC circuit, resonance occurs at only one specific frequency. A formula for this resonant frequency is developed as follows:

Substitute the reactance formulas, and solve for the resonant frequency, ๐‘“๐‘Ÿ

Take the square root of both sides. The formula for resonant frequency is

Series Resonance

Page 11: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 11

Exercice

Page 12: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 12

Frequency Response

Page 13: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 13

The general shape of the impedance versus frequency for a series RLC circuit is superimposed on the curves for XL and XC. Notice that at the resonant frequency, the circuit is resistive, and Z = R

Impedance of series RLC circuits

Page 14: Chapter 14: RLC Circuits and Resonance

Learning with PurposeSlide 14

Summary of important concepts for series resonance:

โ€ข Capacitive and inductive reactances are equal.

โ€ข Total impedance is a minimum and is resistive.

โ€ข The current is maximum.

โ€ข The phase angle between VS and IS is zero.

โ€ข ๐‘“๐‘Ÿ is given by ๐‘“๐‘Ÿ =1

2๐œ‹ ๐ฟ๐ถ

Series Resonance

Summary