Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers...

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Electronics Electronics Principles & Applications Principles & Applications Sixth Edition Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A. Schuler

Transcript of Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers...

Page 1: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

ElectronicsElectronics

Principles & ApplicationsPrinciples & ApplicationsSixth EditionSixth Edition

Chapter 7More About

Small-Signal Amplifiers(student version)

©2003 Glencoe/McGraw-Hill

Charles A. Schuler

Page 2: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

• Amplifier Coupling

• Voltage Gain

• FET Amplifier

• Negative Feedback

• Frequency Response

INTRODUCTION

Page 3: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Dear Student:

This presentation is arranged in segments. Each segment is preceded by a Concept Preview slide and is followed by a Concept Review slide. When you reach a Concept Review slide, you can return to the beginning of that segment by clicking on the Repeat Segment button. This will allow youto view that segment again, if you want to.

Page 4: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Preview• Cascade amplifiers can use capacitive coupling.

• When dc gain is required, direct coupling is required.

• The Darlington configuration is an example of direct coupling.

• Transformer coupling offers the advantage of impedance matching.

• The impedance ratio is equal to the square of the turns ratio.

• Tuned transformers provide selectivity.

Page 5: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

These two points are at different dc voltages.

Capacitive coupling is convenient in cascade ac amplifiers.

Page 6: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

Direct coupling is required for dc gain.

Page 7: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

The darlington is a popular dc arrangement.

Page 8: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

P S

10:1

10 ZRATIO = TRATIO

2

= 102 = 100

ZCOLLECTOR = 100 x 10 = 1000

Transformer coupling offers the advantage of impedance matching.

Page 9: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

Transformer coupling can beused in bandpass amplifiers

to achieve selectivity.

fR

Gain

Page 10: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Amplifier Coupling Quiz

Capacitive coupling is not useful for_________ amplifiers. dc

Dc frequency response requires ________ coupling. direct

Transformer coupling offers the advantage of _________ matching. impedance

Tuned transformer coupling provides frequency _____________. selectivity

A darlington amplifier is an example of _________ coupling. direct

Page 11: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Review• Cascade amplifiers can use capacitive coupling.

• When dc gain is required, direct coupling is required.

• The Darlington configuration is an example of direct coupling.

• Transformer coupling offers the advantage of impedance matching.

• The impedance ratio is equal to the square of the turns ratio.

• Tuned transformers provide selectivity.

Repeat Segment

Page 12: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Preview

• The input impedance of a C-E amplifier is equal to the equivalent parallel resistance of the base divider and rin of the transistor.

• rin is times the sum of the emitter resistances when the emitter resistor is not bypassed.

• Loading the output circuit changes the clipping points and decreases the voltage gain.

• The clipping points are shown by the ac load line.

• The ac load line passes through the same Q-point as the dc load line.

Page 13: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

EB

C

RL

VCC

RB2 RE

= 12 V

2.7 k

22 k = 2.2 k

More about solving the practical circuit for its ac conditions:

= 220

Zin = ?

Page 14: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

EB

C

RL

VCC

RB2 RE

= 12 V

2.7 k

22 k = 2.2 k

Zin is a combination of RB1, RB2, and rin of the transistor.

= 220

rin = (RE + rE)

rin = (220 + 9.03 )

rin = 34.4 k

Note: rin = rE

when RE is bypassed.

Determine rin first:

Page 15: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

EB

C

RL

VCC

RB2 RE

= 12 V

2.7 k

22 k = 2.2 k

= 220

Zin =1

RB2

1rin

1+

RB1

1+

++Zin =

1

2.7 k1

34.4 k1

22 k1

Zin = 2.25 k

RB1, RB2, and rin act in parallelto load the input signal.

Page 16: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

VCC

RB2 RE

= 12 V

2.7 k

22 k RL= 2.2 k

= 220

Load = 2.2 k

What happens when an amplifier is loaded?

RL and the Load act in parallel.

RP = 1.1 k

Page 17: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

RB2 RE

VCC = 12 V

2.7 k

22 k RL= 2.2 k

= 220

Load = 2.2 k

There are two saturation currents for a loaded amplifier.

RP = 1.1 k

ISAT(DC) = VCC

RL + RE

= 4.96 mA

ISAT(AC) = VCC

RP + RE

= 9.09 mA

Page 18: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0 2 4 6 8 10 12 14 16 18

2468

101214

VCE in Volts

IC in mA

20 A

0 A

100 A

80 A

60 A

40 A

There are two load lines for a loaded amplifier.

DC

TEMPORARY AC

The DC load line connects VCC and ISAT(DC).

A temporary AC load line connects VCC and ISAT(AC).

Page 19: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0 2 4 6 8 10 12 14 16 18

2468

101214

VCE in Volts

IC in mA

20 A

0 A

100 A

80 A

60 A

40 A

5.3 V

DC

AC

TEMP. AC

The quiescent VCE is projected to the DC load line to establish the Q-point. The AC load line is drawn through

the Q-point, parallel to the temporary AC load line.

Page 20: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0 2 4 6 8 10 12 14 16 18

2468

101214

VCE in Volts

IC in mA

20 A

0 A

100 A

80 A

60 A

40 A

5.3 V

AC

The AC load line shows the limits for VCE and if the Q-point is properly located.

With loaded amplifiers, the Q-point is often closer to saturation.

Page 21: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

RB1

RB2 RE

VCC = 12 V

2.7 k

22 k RL= 2.2 k

= 220

Load = 2.2 k

What about voltage gain for a loaded amplifier?

RP = 1.1 k

AV =RP

RE + rE

AV =1.1 k

220 9.03= 4.8

Page 22: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

VCC

Zin of the 2nd stage loads the 1st stage.

When analyzing cascade amplifiers, remember:

2nd1st

Page 23: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Amplifier ac Conditions Quiz

Emitter bypassing _________ an amplifier’s input impedance.

decreases

Loading at the output of an amplifier________ its voltage gain. decreases

A loaded amplifier has two load lines: dc and ___________. ac

The clipping points of a loaded amplifier are set by its _______ load line. ac

In a cascade amplifier, the Zin of a stage _______ the prior stage. loads

Page 24: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Review• The input impedance of a C-E amplifier is

equal to the equivalent parallel resistance of the base divider and rin of the transistor.

• rin is times the sum of the emitter resistances when the emitter resistor is not bypassed.

• Loading the output circuit changes the clipping points and decreases the voltage gain.

• The clipping points are shown by the ac load line.

• The ac load line passes through the same Q-point as the dc load line.

Repeat Segment

Page 25: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Preview• A common-source JFET amplifier uses the gate

as the input and the drain as the output.

• The forward transfer admittance (Yfs) can be determined from the drain family of curves.

• Voltage gain is equal to Yfs times RL.

• Source bias produces negative feedback and decreases the voltage gain.

• The gain with feedback is determined by the feedback ratio and the open-loop gain.

• The feedback can be eliminated with a source bypass capacitor.

Page 26: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Drain

Source

Gate

VDD = 20 V

VGS = 1.5 V

RGCC

RL = 5 k

Inputsignal

Common-source JFET amplifier.

Fixed bias

ISAT = 20 V

5 k= 4 mA

Phase-invertedoutput

Page 27: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0

2

4

1

VDS in Volts

ID in mA

5 10 15 20 25

3

-2.5

-2.0

-1.5

-1.0

-0.5

0

N-channel JFET characteristic curves

VG

S in

Vol

ts

Load line

The Q-point is set by the fixed bias.

8 VP-P

1 VP-P

AV = 8

Page 28: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0

2

4

1

VDS in Volts

ID in mA

5 10 15 20 25

3

-2.5

-2.0

-1.5

-1.0

-0.5

0Determining forward transfer admittance:

Yfs = ID

VGS

VG

S in

Vol

ts

VDS

1.6 mA

= 1.6 mS

Page 29: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

D

S

G

VDD = 20 V

VGS = 1.5 V

RGCC

RL = 5 k

When the forward transfer admittance is known,the voltage gain can be determined using:

AV = Yfs x RL

= 1.6 mS x 5 k

= 8

This agrees with the graphic solution.

Page 30: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

D

S

G

VDD

VGS = ID x RS

RGCC

RL

RS

Source bias eliminates the need for a separate VGS supply.

IS = ID

This resistor also providesac negative feedback whichdecreases the voltage gain.

Page 31: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Vin - BVout

A(Vin - BVout)

BVout

A = open loop gain

Summingjunction

Vin VoutA

B Feedback

A negative feedback model

B = feedback ratio

Vout = A(Vin - BVout)Vout = AVin - ABVout

AVin

Vout

1 = - ABAVin

Vout

AB +1 =Vin

Vout

AB +1A

=Vin

Vout

AB +1

A=

AB +1AVin Vout

A simplified model

Page 32: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

D

S

G

VDD

RGCC

RL

RS

= 5 k

= 800

The feedback ratio (B) for this circuitis easy to determine since the source and

drain currents are the same.

B = 800 5 k

= 0.16

Page 33: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

AB +1AVin Vout

Use the simplified model:

A(WITH NEG. FEEDBACK) =8

(8)(0.16) + 1= 3.51

Page 34: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

CS

DG

VDD

RGCC

RL

RS

The source bypass capacitor will eliminate the ac negative feedback

and restore the voltage gain.

Page 35: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

JFET Amplifier Quiz

In a common-source amplifier, the input signal goes to the _______. gate

In a common-source amplifier, the inputto output phase relationship is ____. 180o

The voltage gain of a C-S amplifier is equal to Yfs x _________. load resistance

Source bias is produced by current flow through the _______ resistor. source

An unbypassed source resistor _______ the voltage gain of a C-S amp. decreases

Page 36: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Review• A common-source JFET amplifier uses the gate

as the input and the drain as the output.• The forward transfer admittance (Yfs) can be

determined from the drain family of curves.• Voltage gain is equal to Yfs times RL.• Source bias produces negative feedback and

decreases the voltage gain.• The gain with feedback is determined by the

feedback ratio and the open-loop gain.• The feedback can be eliminated with a source

bypass capacitor.

Repeat Segment

Page 37: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Preview

• Dc negative feedback stabilizes the Q-point.

• Ac negative feedback decreases gain.

• Ac negative feedback increases bandwidth.

• Ac negative feedback reduces distortion.

• Amplifier gain is maximum at mid-band.

• The break frequencies are where the gain drops by 3 dB.

• Amplifier bandwidth is found by subtracting the lower break frequency from the upper break frequency.

Page 38: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Amplifier Negative Feedback

• DC reduces sensitivity to device parameters

• DC stabilizes operating point

• DC reduces sensitivity to temperature change

• AC reduces gain

• AC increases bandwidth

• AC reduces signal distortion and noise

• AC may change input and output impedances

Page 39: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

0.707 Amax

A

f

The frequency response curve of an ac amplifier

Bandwidth

The gain is maximum in the midband.

Amax

Midband

The bandwidth spans the -3 dB points which are called the break frequencies.

-3dB

Page 40: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

50

10 F

10 F

1 k

100 1k

6.8 k

The emitter bypass capacitor in this amplifier hasa significant effect on both gain and bandwidth.

Page 41: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Gai

n in

dB

0

50

Frequency10 Hz 100 MHz

BW1

BW2

Gain and bandwidth with and without the emitter bypass

Page 42: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Amplifier Frequency Response

• The lower break frequency is partly determined by coupling capacitors.

• It is also influenced by emitter bypass capacitors.

• The upper break frequency is partly determined by transistor internal capacitance.

• Both break frequencies can be influenced by negative feedback.

Page 43: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

Concept Review• Dc negative feedback stabilizes the Q-point.

• Ac negative feedback decreases gain.

• Ac negative feedback increases bandwidth.

• Ac negative feedback reduces distortion.

• Amplifier gain is maximum at mid-band.

• The break frequencies are where the gain drops by 3 dB.

• Amplifier bandwidth is found by subtracting the lower break frequency from the upper break frequency.

Repeat Segment

Page 44: Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.

REVIEW

• Amplifier Coupling

• Voltage Gain

• FET Amplifier

• Negative Feedback

• Frequency Response