26
1 Resonant Circuits Resonant Circuits SEE 1023 Circuit Theory SEE 1023 Circuit Theory Frequency Response Frequency Response

Resonant Circuits

Embed Size (px)

DESCRIPTION

Resonant Circuits. SEE 1023 Circuit Theory. Frequency Response. L. R. I. + V L -. + V R -. + V C -. V s. C. w (varied). Series RLC Circuit. When w varies, the impedance of the circuit will vary. Then, the current and the real power will also vary. - PowerPoint PPT Presentation

Citation preview

Page 1: Resonant Circuits

1

Resonant CircuitsResonant Circuits

SEE 1023 Circuit TheorySEE 1023 Circuit Theory

Frequency ResponseFrequency Response

Page 2: Resonant Circuits

2

Series RLC Circuit

When varies, the impedance of the circuit will vary.Then, the current and the real power will also vary.

We would like to study the frequency response of these quantities.

Vs

R L

C

I

+ VR -+ VL -

+

VC

-

(varied)

Page 3: Resonant Circuits

3

Series RLC Circuit

Impedance as a function of frequency: )1

()(C

LjRZ

Current as a function of frequency: I Vs

R2 L1

C

2

Power as a function of frequency: P Vs

2

R2 L1

C

2

R

Reactance as a function of frequency: X L1

C

Page 4: Resonant Circuits

4

Series RLC Circuit

Excitation(Input)

Response(Output)

Series RLC Circuit

Constant input voltage: VsVariable Source angular frequency:

Main response: current

Other responses: Power, Impedance, reactance, etc.

Page 5: Resonant Circuits

5

Series RLC Circuit in PSpice

It is too hard to study the frequency response of these quantities manually.

Vs

R L

C

I

+ VR -+ VL -

+

VC

-

(varied)

It is too easy to study the frequency response of these quantities PSpicely.

0

1

2 3

Page 6: Resonant Circuits

6

Series RLC Circuit in PSpice

Series resonant CircuitVs 1 0 AC 10VR1 1 2 10L1 2 3 100mHC1 3 0 10uF.AC LIN 1001 100Hz 220Hz.Probe.end

Start FREQ.

End FREQ.Total PTS.To Displaygraph

Page 7: Resonant Circuits

7

In the Probe windows

Trace Expression

M(V(1)/I(R1)) Magnitude of Z

Response

P(V(1)/I(R1)) Phase of Z

R(V(1)/I(R1)) Real part of Z

IMG(V(1)/I(R1)) Imaginary part of Z

Page 8: Resonant Circuits

8

In the Probe windows

Trace Expression

M(I(R1)) Magnitude of I

Response

P(I(R1)) Phase of I

R(I(R1)) Real part of I

IMG(I(R1)) Imaginary part of I

Page 9: Resonant Circuits

9

In the Probe windows

Trace Expression

V(1,2) Magnitude of VR

Response

V(2,3) Magnitude of VL

V(3) Magnitude of VC

I(R1)*I(R1)*10 Real power, P

Page 10: Resonant Circuits

10

Run Pspice File

Frequency Response of The Current

Page 11: Resonant Circuits

11

800 840 880 920 960 1000 1040 1080 1120 1160 12000.22

0.41

0.61

0.81

1

1.2

I ( )

(Variation of the current with frequency)

Frequency Response of The Current

At Resonance, the current is maximumAt Resonance, the current is maximum

Page 12: Resonant Circuits

12

Basic Questions

What is the minimum value of Z?

What is the maximum value of I?

What is the maximum value of P?

Z= R

R

VII so

R

VRIPP s

oo

22

Page 13: Resonant Circuits

13

Basic Questions

The magnitude of I?

When the power P = Po/2, what is

The magnitude of Z?

The magnitude of X?

The angular frequency?

1 lower half power frequency

2 higher half power frequency

R

VI s

21

RZ 2

RX RX

at 1

at 2

Page 14: Resonant Circuits

14

Resonant Condition

By definition the resonant angular frequency, o, for the RLC series circuit occurs at the peak of the current response. Under this condition:

The real power is maximum The magnitude of impedance is minimum The circuit is purely resistive The imaginary part of the impedance is zero The pf = 1 The current is in phase with the voltage source

Page 15: Resonant Circuits

15

Lower half-power angular frequency, 1, condition

By definition lower half-power angular frequency, 1, occurs when the power is Po/2 and the angular frequency is below the resonant angular frequency.

The real power is Po/2 The current is Io /2 The magnitude of impedance is 2R X = -R The circuit is predominantly capacitive The pf = cos(45) leading

Page 16: Resonant Circuits

16

By definition lower half-power angular frequency, 2, occurs when the power is Po/2 and the angular frequency is above the resonant angular frequency.

The real power is Po/2 The current is Io /2 The magnitude of impedance is 2R X = +R The circuit is predominantly inductive The pf = cos(45) lagging

Lower half-power angular frequency, 2, condition

Page 17: Resonant Circuits

17

The Voltage Phasor Diagram at o

For R: I is in phase with VR

For L: I lags VL by 90

For C: I leads VC by 90

For series circuit, use I as the

reference. VR = VSI

VL

VC

at o

The circuit is purely resistive.

Page 18: Resonant Circuits

18

The Voltage Phasor Diagram at 1

For R: I is in phase with VR

For L: I lags VL by 90

For C: I leads VC by 90

For series circuit, use I as a

reference.

VS

I

VL

VL+VC

at 1

VR

VC

The circuit is predominantly capacitive.

Page 19: Resonant Circuits

19

The Voltage Phasor Diagram at 2

For R: I is in phase with VR

For L: I lags VL by 90

For C: I leads VC by 90

For series circuit, use I as the

reference.

VS

I

VL

VL+VC

at 2

VR

VC

The circuit is predominantly inductive.

Page 20: Resonant Circuits

20

Learning Sheet 3

Five Resonant Parameters:

1. Resonant Angular frequency,

2. Lower cut-off angular frequency,

4. Bandwidth of the resonant circuit,

3. Upper cut-off angular frequency,

5. Quality factor of the resonant circuit,

o

1

2

BW

Q

Page 21: Resonant Circuits

21

Learning Sheet 3

Five Resonant Parameters:

1. Resonant Angular frequency,

2. Lower cut-off angular frequency,

4. Bandwidth of the resonant circuit,

3. Upper cut-off angular frequency,

5. Quality factor of the resonant circuit,

LCo

1

LCL

R

L

R 1

22

2

1

LCL

R

L

R 1

22

2

2

L

RBW

C

L

RR

LQ o 1

Note: Lower cut-off angular frequency is also popularly known aslower half-power angular frequency. The same is true for the upper.

Page 22: Resonant Circuits

22

Learning Sheet 3

We know that,

Lower cut-off angular frequency,

Upper cut-off angular frequency,

LCL

R

L

R 1

22

2

1

LCL

R

L

R 1

22

2

2

Are the half-power frequencies symmetrical around o?

21 o

Generally No.

The resonant frequency is the geometric mean of the half-power frequencies.

But, If Q 10, the half-power frequencies can be approximately considered as symmetrical around o . Then

21

BWo

22

BWo and

Page 23: Resonant Circuits

23

Example: Series RLC Resonant Circuit

Vs = 10 Vrms, R = 10 , L = 100 mH, C = 10 F

Vs

R L

C

I

+ VR -+ VL -

+

VC

-

(varied)

Page 24: Resonant Circuits

24

Find:

(ii) The magnitude of the current at o

(iii) The real power P at o

(iv) The expression for i(t) at o

(v) The expression for vL(t) and vC(t) at o

(i) The impedance of the circuit at o

(vii) The current at 1 in polar form

(viii) The real power P at 1

(ix) The expression for i(t) at 1

(x) The expression for vC(t), vL(t) and vC(t)+vL(t) at 1

(vi) The impedance of the circuit at 1 in polar form

Page 25: Resonant Circuits

25

(xii) The current at 2 in polar form

(xiii) The real power P at 2

(xiv) The expression for i(t) at 2

(xv) The expressions for vL(t), vC(t) and vL(t)+vC(t) at 2

(xi) The impedance of the circuit at 2 in polar form

(xvi) Draw the voltage phasor diagram at o

(xvii) Draw the voltage phasor diagram at 1

(xviii) Draw the voltage phasor diagram at 2

(ixx) Draw the waveforms of vC(t), vL(t) and vC(t)+vL(t) at o

(xx) Draw the waveforms of vC(t), vL(t) and vC(t)+vL(t) at 1

(xxi) Draw the waveforms of vL(t), vC(t) and vL(t)+vC(t) at 2

Page 26: Resonant Circuits

26

(xxii) The resonant frequency, fo

(xxiii) The lower cut-off frequency, f1

(xxiv) The upper cut-off frequency, f2

(xxv) The bandwidth, BW in Hertz

(xxvi) The Quality factor, Q