ele1110c tutorial 3 27/09/2006 27/09/2006 cathy, kai caihong

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ELE1110C Tutorial 3 ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong Cathy, KAI Caihong

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Page 1: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

ELE1110C Tutorial 3ELE1110C Tutorial 3

27/09/200627/09/2006Cathy, KAI CaihongCathy, KAI Caihong

Page 2: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

OutlineOutline

• Lecture Reviews

• Examples

Page 3: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

How to represent a sine wave How to represent a sine wave (sinusoid)?(sinusoid)?

• Complex number notation (L2.137)– a+jb

Represent a vector with a magnitude and phase

– Magnitude =

– Phase =

– Unit vector =

a

jb22 ba

ab

tan 1

cos sinj 1

,1sinjcose j

Page 4: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• Rotation: multiplied by j (rotate anti-clockwise)

22 2 , cos sin cos sin , . .

j tj tLet t then t j t t j t i e e e

• => Period = 2π/w, Frequency = 1/Period = w/2π• => w : Angular Frequency (i.e. w = 1000 x 2π

for a 1000Hz sine wave)

Page 5: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Impedance CalculationImpedance Calculation• Capacitor:

( . . )

/ *

/ / 1/

j t

j t

c

Let V Ae i e V A

I CdV dt C j Ae j C V

Z V I V j CV j C

Page 6: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Impedance CalculationImpedance Calculation• Impedance of capacitor:

• Magnitude of impedance :

• Low frequency => ZC is large => open circuit

• High frequency => ZC is small => short circuit

1 C

VZ

I jwC

1CZ Cw

Page 7: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Circuit AnalysisCircuit Analysis

• If V1 is an varying voltage, what is V2?

R

C V2V1

Page 8: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Capacitor – Capacitor – Transfer FunctionTransfer Function• Definition

– Impedance of capacitor :

• By KVL

• So that

• Hence

2C

VZ

I

1 2 CV IR V IR IZ

1

1

C

I VR Z

2 1 1 1

1/ 1

1/ 1

C

CC

Z j CV IZ V V V

R Z R j C j CR

Page 9: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Capacitor – Capacitor – Transfer FunctionTransfer Function• Transfer function T(w)= Output / Input

=

• Note that the output response depends on the frequency of the input sinusoid

• High frequency ( ),– High frequency signals are cut

• Low frequency ( ), – Low frequency signals are passed – The circuit is a low pass filter

2

1

( ) 1

( ) 1

V w

V w jwCR

w 2 ( ) 0V w

0w 2 ( ) 1V w

Page 10: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• Usually we focus more on power ration in filter design:

2 2

1 1

1 ( )1out

in

P

P CRj CR

• Therefore, 3dB point (half-power, or cut-off point):

120.5 / 1 ( )out inP P CR

Page 11: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• At half power point,

=> CCR = 1

=> C = 1/RC

• since C = 2f , therefore fC = 1/2RC

2

1 1 1

2 21 ( )OUT

IN

V

V wCR

33dB point of a LPFdB point of a LPF

Page 12: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Magnitude and phase response of a low pass filter Magnitude and phase response of a low pass filter (LPF)(LPF)

– Magnitude response =

– Phase response =

2IN

OUT

)wCR(1

1VV

)wCR(tanVV 1

IN

OUT

Page 13: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• dB is the logarithm of a ratio between powers

– 3dB => POUT is 2 times PIN

– 10dB => POUT is 10 times PIN

– 20dB => POUT is 100 times PIN

– -3dB => POUT is half of PIN , and so on

IN

OUT

P

Plog10dB

Page 14: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Examples from Problem Sheet 3

• Example 1:• Find the transfer function of the following circuit

VOUTC

R1

VIN

R2

Page 15: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• Let Y = (1/ jwC)

• As no current will flow into R2, V1 = Vout, I2 = 0• I0 = I1 = Vin/(R1 + Y)• Vout = V1 = I0 * Y =YVin/(R1+Y)• Then you can find Vout/Vin

Page 16: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Example 2:

• Find the transfer function of the circuit below.

Page 17: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• Let Y1 = (1/ jwC1), Y2 = (1/ jwC2)

• V1 = Vin*(Y1//(Y2+R2)) / ( (Y1//(Y2+R2)) + R1)

• Vout = V1*(R2/(R2+Y2))

• Therefore, Vout = [Vin*(Y1//(Y2+R2)) / ( (Y1//(Y2+R2)) + R1) ] *(R2/(R2+Y2))

• (Vout/Vin )= (Y1//(Y2+R2)) *(R2/(R2+Y2)) / ( (Y1//(Y2+R2)) + R1) *(R2/(R2+Y2))

Page 18: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

Example 3:

• The following diagram shows an elevator call button - an example of proximity switch. The button has two sides separated by insulator. One side is a plate conductor and the other side is a ring conductor. The button behaves as a capacitor (C1). When a finger is placed somewhere near the middle of the ring, the finger acts like an earth as the body can absorb a fair amount of charges quickly. The capacitance between the ring and the finger is C2 and the capacitance between the plate and the finger is C3. Also shown are the equivalent circuits for the two states.

Page 19: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong
Page 20: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• The circuit for the elevator call button is as follows.

• Suppose C1=30pF, and C2=C3=10pF, find V with i) no finger present, and ii) finger present.

Page 21: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• As Q = CV, we can deduce that the ratio of voltage across 2 capacitors in series is:

1)

, A BA A B B

B A

V CC V C V

V C

301, ,

30

2

AA B s

B

sA B

VV V V

V

VV V

Page 22: ELE1110C Tutorial 3 27/09/2006 27/09/2006 Cathy, KAI Caihong

• 2) As no current will flow into the earth point (finger), the earthing has no effect to this circuit.

11 1

30, 30 30 5 35,10 10

35, ,

30

6 7,

13 13

B A

BA B S

A

A S B s

C C

VV V V

V

V V V V