Electronics Principles Applications Sixth Edition Charles A Schuler

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Electronics Principles & Applications Sixth Edition Charles A. Schuler Chapter 9 Operational Amplifiers ©

Electronics Principles & Applications Sixth Edition Charles A. Schuler Chapter 9 Operational Amplifiers © 2003 Glencoe/Mc. Graw-Hill

INTRODUCTION • The Differential Amplifier • The Operational Amplifier • Determining Gain • Frequency

INTRODUCTION • The Differential Amplifier • The Operational Amplifier • Determining Gain • Frequency Effects • Applications • Comparators

A differential amplifier driven at one input +VCC Inverted output B Noninverted output C

A differential amplifier driven at one input +VCC Inverted output B Noninverted output C E -VEE B

Both outputs are active because Q 1 drives Q 2. Q 1 serves as

Both outputs are active because Q 1 drives Q 2. Q 1 serves as an emitter-follower amplifier in this mode to drive Q 2. +VCC C B Q 1 E Q 2 serves as a common-base amplifier in this mode. It’s driven at its emitter. C E Q 2 -VEE B

A differential amplifier driven at both inputs Common mode input signal +VCC Reduced output

A differential amplifier driven at both inputs Common mode input signal +VCC Reduced output B Reduced output C E -VEE B

A differential amplifier driven at both inputs Differential mode input signal +VCC Increased output

A differential amplifier driven at both inputs Differential mode input signal +VCC Increased output B Increased output C E -VEE B

Differential Amplifier dc Analysis IR = VEE - VBE RE E IE = IR

Differential Amplifier dc Analysis IR = VEE - VBE RE E IE = IR 2 E 9 V - 0. 7 V = 2. 13 m. A = 3. 9 k. W VCC = 1. 06 m. A 4. 7 k. W IC = IE = 1. 06 m. A 10 k. W B RB +9 V RL RL C E 3. 9 k. W VEE VR = I C x RL L = 1. 06 m. A x 4. 7 k. W = 4. 98 V VCE = VCC - VRL - VE 4. 7 k. W = 9 - 4. 98 -(-0. 7) C E RE -9 V = 4. 72 V B RB 10 k. W

Differential Amplifier dc Analysis (continued) Assume b = 200 IB = IC b VB

Differential Amplifier dc Analysis (continued) Assume b = 200 IB = IC b VB = V R = I B x RB B 1. 06 m. A = 200 = 5. 3 m. A VCC 4. 7 k. W 10 k. W RB +9 V = 53 m. V RL RL 4. 7 k. W C B = 5. 3 m. A x 10 k. W E 3. 9 k. W VEE C E RE -9 V B RB 10 k. W

Differential Amplifier ac Analysis 50 m. V (50 m. V is conservative) = 47

Differential Amplifier ac Analysis 50 m. V (50 m. V is conservative) = 47 W = r. E = IE 1. 06 m. A RL VCC +9 V AV(CM) = RL 2 x RE AV(DIF) = 2 x r. E 4. 7 k. W RL RL 4. 7 k. W = 4. 7 k. W 2 x 3. 9 k. W = = 50 2 x 47 W C C = 0. 6 10 k. W B RB E 3. 9 k. W VEE E RE -9 V B RB 10 k. W

Differential Amplifier ac Analysis (continued) CMRR = 20 x log AV(DIF) AV(CM) VCC 4.

Differential Amplifier ac Analysis (continued) CMRR = 20 x log AV(DIF) AV(CM) VCC 4. 7 k. W 10 k. W RB +9 V RL RL 4. 7 k. W C B 50 = 20 x log = 38. 4 d. B 0. 6 E 3. 9 k. W VEE C E RE -9 V B RB 10 k. W

AV(CM) = A current source can replace RE to decrease the common mode gain.

AV(CM) = A current source can replace RE to decrease the common mode gain. RL VCC 2 x RE Replaces this with a very high resistance value. 10 k. W 4. 7 k. W RL RL 4. 7 k. W C B RB E * C E B RB 10 k. W 2 m. A *NOTE: Arrow shows conventional current flow.

A Practical Current Source IC 9 V - 5. 1 V IZ = =

A Practical Current Source IC 9 V - 5. 1 V IZ = = 10 m. A 390 W IE = 390 W 5. 1 V - 0. 7 V 2. 2 k. W IC = IE = 2 m. A 5. 1 V 2. 2 k. W -9 V = 2 m. A

A Demonstration of Common-mode Rejection The common-mode signal cannot be seen in the output.

A Demonstration of Common-mode Rejection The common-mode signal cannot be seen in the output. The amplitude of the common-mode signal is almost 30 times the amplitude of the differential signal. 6. 3 V 60 Hz 212 m. V 1 k. Hz

Differential Amplifier Quiz When a diff amp is driven at one input, the number

Differential Amplifier Quiz When a diff amp is driven at one input, the number of active outputs is _____. two When a diff amp is driven at both inputs, there is high gain for a _____ signal. differential When a diff amp is driven at both inputs, there is low gain for a ______ signal. common-mode The differential gain can be found by dividing the collector load by ____. 2 r. E The common-mode gain can be found by dividing the collector load by ____. 2 RE

Op amps have two inputs Inverting input Non-inverting input Output

Op amps have two inputs Inverting input Non-inverting input Output

Op-amp Characteristics • High CMRR • Available as ICs • High input impedance •

Op-amp Characteristics • High CMRR • Available as ICs • High input impedance • Inexpensive • High gain • Widely applied • Low output impedance • Reliable

With both inputs grounded through equal resistors, VOUT should be zero volts. +VCC VOUT

With both inputs grounded through equal resistors, VOUT should be zero volts. +VCC VOUT -VEE Imperfections can make VOUT non-zero. The offset null terminals can be used to zero VOUT.

Dt DV 741 DV Slew rate = Dt 0. 5 V ms The output

Dt DV 741 DV Slew rate = Dt 0. 5 V ms The output of an op amp cannot change instantaneously.

VP f > f. MAX = Slew-rate distortion Slew Rate 2 p x VP

VP f > f. MAX = Slew-rate distortion Slew Rate 2 p x VP

Operational Amplifier Quiz The input stage of an op amp is a _____ amplifier.

Operational Amplifier Quiz The input stage of an op amp is a _____ amplifier. differential Op amps have two inputs: one is inverting and the other is ____. noninverting An op amp’s CMRR is a measure of its ability to reject a ____ signal. common-mode The offset null terminals can be used to zero an op amp’s _____. output The ability of an op amp output to change rapidly is given by its _____. slew rate

Op-amp Follower AV(OL) = the open loop voltage gain AV(CL) = the closed loop

Op-amp Follower AV(OL) = the open loop voltage gain AV(CL) = the closed loop voltage gain This is a closed-loop circuit with a voltage gain of 1. It has a high input impedance RL and a low output impedance.

Op-amp Follower AV(OL) = 200, 000 AV(CL) = 1 The differential input approaches zero

Op-amp Follower AV(OL) = 200, 000 AV(CL) = 1 The differential input approaches zero due to the high open-loop gain. Using this model, VOUT = VIN. VDIF = 0 VIN VOUT RL

Op-amp Follower AV(OL) = 200, 000 B=1 A AB +1 VIN VOUT The feedback

Op-amp Follower AV(OL) = 200, 000 B=1 A AB +1 VIN VOUT The feedback ratio = 1 200, 000 @1 AV(CL) = (200, 000)(1) + 1 VIN VOUT RL

The closed-loop gain is increased by decreasing the feedback with a voltage divider. R

The closed-loop gain is increased by decreasing the feedback with a voltage divider. R 1 200, 000 AV(CL) = = 11 (200, 000)(0. 091) + 1 RF R 1 B= 100 k. W RF + R 1 10 k. W = VIN VOUT RL 10 k. W 100 k. W + 10 k. W = 0. 091

It’s possible to develop a different model for the closed loop gain by assuming

It’s possible to develop a different model for the closed loop gain by assuming VDIF = 0. R 1 VIN = VOUT x R 1 + R F RF Divide both sides by VOUT and invert: 100 k. W R 1 10 k. W VOUT VDIF = 0 VIN VOUT RL VIN RF =1+ R 1 AV(CL) = 11

In this amplifier, the assumption VDIF = 0 leads to the conclusion that the

In this amplifier, the assumption VDIF = 0 leads to the conclusion that the inverting op amp terminal is also at ground potential. This is called a virtual ground. Virtual ground RF We can ignore the op amp’s input current since it is so small. Thus: IR = I R 1 10 k. W R 1 By Ohm’s Law: 1 k. W VIN VDIF = 0 VIN F VOUT R 1 RL VOUT VIN = = -VOUT RF -R F R 1 = -10 The minus sign designates an inverting amplifier.

Due to the virtual ground, the input impedance of the inverting amplifier is equal

Due to the virtual ground, the input impedance of the inverting amplifier is equal to R 1. Virtual ground RF 10 k. W R 1 1 k. W VDIF = 0 VIN Although op amp input currents are small, in some applications, offset error is minimized by providing equal paths for the input currents. R 2 = R 1 || RF = 910 W This resistor reduces offset error.

A typical op amp has internal frequency compensation. R C Output Break frequency: 1

A typical op amp has internal frequency compensation. R C Output Break frequency: 1 f. B = 2 p. RC

Bode Plot of a Typical Op Amp Break frequency 120 100 80 Gain in

Bode Plot of a Typical Op Amp Break frequency 120 100 80 Gain in d. B 60 40 20 0 1 10 100 1 k 100 k 1 M Frequency in Hz

Op amps are usually operated with negative feedback (closed loop). This increases their useful

Op amps are usually operated with negative feedback (closed loop). This increases their useful frequency range. AV(CL) = RF VIN RF =1+ R 1 100 k. W =1+ = 101 1 k. W 100 k. W R 1 1 k. W VOUT d. B Gain = 20 x log 101 = 40 d. B VIN VOUT RL

Using the Bode plot to find closed-loop bandwidth: 120 100 Gain in d. B

Using the Bode plot to find closed-loop bandwidth: 120 100 Gain in d. B 80 Break frequency 60 AV(CL) 40 20 0 1 10 100 1 k 100 k 1 M Frequency in Hz

A 741 op amp slews at 0. 5 V ms 70 V A 318

A 741 op amp slews at 0. 5 V ms 70 V A 318 op amp slews at ms There are two frequency limitations: Slew rate determines the large-signal bandwidth. Internal compensation sets the small-signal bandwidth.

The Bode plot for a fast op amp shows increased small-signal bandwidth. 120 100

The Bode plot for a fast op amp shows increased small-signal bandwidth. 120 100 80 Gain in d. B 60 40 f. UNITY 20 0 1 10 100 1 k 100 k 1 M 10 M Frequency in Hz

f. UNITY can be used to find the small-signal bandwidth. AV(CL) = RF VIN

f. UNITY can be used to find the small-signal bandwidth. AV(CL) = RF VIN RF =1+ R 1 100 k. W =1+ = 101 1 k. W 100 k. W R 1 1 k. W VIN VOUT 318 Op amp RL f. UNITY f. B = AV(CL) 10 MHz = = 99 k. Hz 101

Op Amp Feedback Quiz The open loop gain of an op amp is reduced

Op Amp Feedback Quiz The open loop gain of an op amp is reduced with _____ feedback. negative The ratio RF/R 1 determines the gain of the ______ amplifier. inverting 1 + RF/R 1 determines the gain of the ______ amplifier. noninverting Negative feedback makes the - input of the inverting circuit a ____ ground. virtual Negative feedback _____ small signal bandwidth. increases

R Amplitude Response of RC Lag Circuit Vout C 1 fb = 2 p.

R Amplitude Response of RC Lag Circuit Vout C 1 fb = 2 p. RC fb 0 d. B Vout -20 d. B -40 d. B -60 d. B 10 fb 1000 fb f

R Phase Response of RC Lag Circuit = tan -1 Vout -45 o -90

R Phase Response of RC Lag Circuit = tan -1 Vout -45 o -90 o C -XC R 0. 1 fb 0 o Vout fb 10 fb f

Interelectrode Capacitance and Miller Effect The gain from base to collector makes CBC effectively

Interelectrode Capacitance and Miller Effect The gain from base to collector makes CBC effectively larger C BE in the input circuit. CBC R CMiller = AVCBC CInput = CMiller + CBE CMiller CBE 1 fb = 2 p. RCInput

Bode Plot of an Amplifier with Two Break Frequencies 50 d. B 40 d.

Bode Plot of an Amplifier with Two Break Frequencies 50 d. B 40 d. B 20 d. B/decade 30 d. B 20 d. B 40 d. B/decade 10 d. B 10 Hz 100 Hz 1 k. Hz fb 1 10 k. Hz 100 k. Hz fb 2

Multiple Lag Circuits: R 1 C 1 R 2 C 2 R 3 0

Multiple Lag Circuits: R 1 C 1 R 2 C 2 R 3 0 o Vout Phase reversal -180 o Negative feedback becomes positive! Vout C 3 f

Op Amp Compensation • Interelectrode capacitances create several break points. • Negative feedback becomes

Op Amp Compensation • Interelectrode capacitances create several break points. • Negative feedback becomes positive at some frequency due to cumulative phase lags. • If the gain is > 0 d. B at that frequency, the amplifier is unstable. • Frequency compensation reduces the gain to 0 d. B or less.

Op Amp Compensation Quiz Beyond fb, an RC lag circuit’s output drops at a

Op Amp Compensation Quiz Beyond fb, an RC lag circuit’s output drops at a rate of _____ per decade. 20 d. B The maximum phase lag for one RC network is _____. 90 o An interelectrode capacitance can be effectively much larger due to _______ effect. Miller Op amp multiple lags cause negative feedback to be ______ at some frequency. positive If an op amp has gain at the frequency where feedback is positive, it will be ______. unstable

Inverted sum of three sinusoidal signals RF 10 k. W 5 k. Hz 3.

Inverted sum of three sinusoidal signals RF 10 k. W 5 k. Hz 3. 3 k. W 1 k. Hz 3 k. Hz Summing Amplifier scaling: 1 k. Hz signal gain is -10 3 k. Hz signal gain is -3 5 k. Hz signal gain is -2

Difference of two sinusoidal signals (V 1 = V 2) RF 1 k. W

Difference of two sinusoidal signals (V 1 = V 2) RF 1 k. W Subtracting Amplifier (A demonstration of common-mode rejection) 1 k. W V 1 V 2 VOUT = V 2 - V 1

A cascade RC low-pass filter (A poor performer since later sections load the earlier

A cascade RC low-pass filter (A poor performer since later sections load the earlier ones. ) An active low-pass filter (The op amps provide isolation and better performance. )

0 Active filter Amplitude in d. B -20 Cascade RC -40 -60 10 100

0 Active filter Amplitude in d. B -20 Cascade RC -40 -60 10 100 Frequency in Hz

Active low-pass filter with feedback VIN C 1 VOUT C 2 feedback At relatively

Active low-pass filter with feedback VIN C 1 VOUT C 2 feedback At relatively low frequencies, Vout and Vin are about the same. Thus, the signal voltage across C 1 is nearly zero. C 1 has little effect at these frequencies.

Active low-pass filter with feedback VIN -3 d. B Gain C 1 VOUT C

Active low-pass filter with feedback VIN -3 d. B Gain C 1 VOUT C 2 Feedback can make a filter’s performance even better! Frequency f C As f. IN increases and C 2 loads the input, Vout drops. This increases the signal voltage across C 1. This sharpens the knee.

0 Active filter using feedback (two stages) Amplitude in d. B -20 -40 -60

0 Active filter using feedback (two stages) Amplitude in d. B -20 -40 -60 10 Note the flat pass band the sharp knee. The slope eventually reaches 24 d. B/octave or 80 db/decade for all the filters (4 RC sections). 100 Frequency in Hz

Active high-pass filter VOUT VIN feedback -3 d. B Gain f. C Frequency

Active high-pass filter VOUT VIN feedback -3 d. B Gain f. C Frequency

VIN VOUT Active band-pass filter (multiple feedback) -3 d. B Gain Bandwidth Frequency

VIN VOUT Active band-pass filter (multiple feedback) -3 d. B Gain Bandwidth Frequency

VOUT VIN Active band-stop filter (multiple feedback) -3 d. B Gain Stopband Frequency

VOUT VIN Active band-stop filter (multiple feedback) -3 d. B Gain Stopband Frequency

56. 6 m. V Active rectifier 0 V 40 m. V 0 V -

56. 6 m. V Active rectifier 0 V 40 m. V 0 V - 56. 6 m. V

Integrator C R VIN V Slope = s VOUT 1 Slope = -VIN x

Integrator C R VIN V Slope = s VOUT 1 Slope = -VIN x RC

Comparator with a 1 Volt Reference +VSAT 1 V 0 V -VSAT VOUT VIN

Comparator with a 1 Volt Reference +VSAT 1 V 0 V -VSAT VOUT VIN 1 V

Comparator with a Noisy Input Signal +VSAT 1 V 0 V -VSAT VOUT VIN

Comparator with a Noisy Input Signal +VSAT 1 V 0 V -VSAT VOUT VIN 1 V

Schmitt Trigger with a Noisy Input Signal +VSAT UTP LTP Trip points: R 1

Schmitt Trigger with a Noisy Input Signal +VSAT UTP LTP Trip points: R 1 VSAT x R 1 + R F -VSAT VIN R 1 VOUT RF Hysteresis = UTP - LTP

+5 V Window Comparator 4. 7 k. W VUL 3 V R 1 311

+5 V Window Comparator 4. 7 k. W VUL 3 V R 1 311 VOUT R 2 4. 7 k. W VIN 311 VLL 1 V VOUT is LOW (0 V) when VIN is between 1 V and 3 V.

Window Comparator VUL 3 V 311 +5 V VOUT VIN 311 VLL Many comparator

Window Comparator VUL 3 V 311 +5 V VOUT VIN 311 VLL Many comparator ICs 1 V require pull-up resistors in applications of this type.

+5 V Window Comparator 4. 7 k. W VUL 3 V R 1 311

+5 V Window Comparator 4. 7 k. W VUL 3 V R 1 311 VOUT R 2 4. 7 k. W VIN 311 VLL 1 V VOUT is TTL logic compatible.

Op Amp Applications Quiz A summing amp with different gains for the inputs uses

Op Amp Applications Quiz A summing amp with different gains for the inputs uses _____. scaling Frequency selective circuits using op amps are called _____ filters. active An op amp integrator uses a _____ as the feedback element. capacitor A Schmitt trigger is a comparator with _____ feedback. positive A window comparator output is active when the input is ______ the reference points. between

REVIEW • The Differential Amplifier • The Operational Amplifier • Determining Gain • Frequency

REVIEW • The Differential Amplifier • The Operational Amplifier • Determining Gain • Frequency Effects • Applications • Comparators