Electronic Circuits for Mechatronics (ELCT 609)...Note that: Q1 and Q2 are matched and Ξ² is large....
Transcript of Electronic Circuits for Mechatronics (ELCT 609)...Note that: Q1 and Q2 are matched and Ξ² is large....
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Electronic Circuits for Mechatronics
(ELCT 609)
Summer 2020 : Round II
Lecture 11: Op-amp Linear and Non-linear
Applications
Course Instructor: Dr. Eman Azab
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Op-amps: IntroductionCircuit Modeling
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Ideal Op-amp Operational amplifiers are
voltage amplifiers with very highgain
Differential Input/Single outputcircuit is the most famous op-amp structure
Ideal op-amp have the followingSpecs:
Infinite Differential voltagegain
Zero Common-modevoltage gain
Infinite Input Resistance
Zero Input Currents
Zero Output Resistance
Infinite Bandwidth (Gain isconstant all over thefrequency Spectrum)
πππ’π‘ = π΄ππ π1 β π2 + π΄ππππ1 + π2
2
π΄ππ = β π΄πππ = 0
π ππ = β π ππ’π‘ = 0
π΄ππ π = πΆπππ π‘.
πππ+ = 0 πππβ = 0
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
3
Operational amplifiers arevoltage amplifiers with very highgain
Differential Input/Single outputcircuit is the most famous op-amp structure
Ideal op-amp have the followingSpecs:
Infinite Differential voltagegain
Zero Common-modevoltage gain
Infinite Input Resistance
Zero Input Currents
Zero Output Resistance
Infinite Bandwidth (Gain isconstant all over thefrequency Spectrum)
πππ’π‘ = π΄ππ π1 β π2 + π΄ππππ1 + π2
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Ideal Op-amp Ideal Op-amp can be modeled using the following circuit:
πππ’π‘ = π΄ππ π1 β π2 + π΄ππππ1 + π2
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π΄ππ = β π΄πππ = 0
π ππ = β π ππ’π‘ = 0
π΄ππ π = πΆπππ π‘.
πππ+ = 0 πππβ = 0Figure from Sedra/Smith Copyright Β© 2010 by Oxford University Press, Inc.
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Non-ideal Op-ampCircuit Realizations of Op-amp
Course Instructor: Dr. Eman Azab
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Ex.: Two stage CMOS Op-amp
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Ex.: BJT 741 Op-amp
Course Instructor: Dr. Eman Azab
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Op-amp Applications
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage Amplifier
Inverting and Non-Inverting Amplifiers
π£ππ£πΌ
= βπ 2π 1
π£ππ£πΌ
= 1 +π 2π 1
Figures from Sedra/Smith Copyright Β© 2010 by Oxford University Press, Inc.
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage Amplifier
Inverting Amplifiers
π£ππ£πΌ
= βπ 2π 1
Course Instructor: Dr. Eman Azab
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Voltage Buffer
Voltage Buffer
The voltage at the input is derived at the output node
without drawing any current from the input source
π£ππ£πΌ
= 1
Figure from Sedra/Smith Copyright Β© 2010 by Oxford University Press, Inc.
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
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Voltage Difference Amplifier
The circuit subtracts two voltage signals
By Applying Superposition principle between π£πΌ1 and π£πΌ2
By Choosing:
π£π = βπ£πΌ1π 2π 1
+ π£πΌ2π 4
π 4 + π 31 +
π 2π 1
π 2π 1
=π 4π 3
π£π =π 2π 1
π£πΌ2 β π£πΌ1
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage Integrator
Inverting configuration with General Impedances
Lossless inverting Integrator
ππππ
= βπ2π1
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage Integrator
Lossy Integrator
DC Gain is defined by:
π£ππ£π
= β
π πΉπ
1 + π πΆπ πΉ
π£ππ£π(0) = β
π πΉπ
Course Instructor: Dr. Eman Azab
Contact: [email protected]
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Summer R2 2020
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Voltage Differentiator
Op-amp based Differentiator
π£ππ£π(π ) = βπ πΆπ
Course Instructor: Dr. Eman Azab
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Voltage Weighted Summer
Figure from Sedra/Smith Copyright Β© 2010 by Oxford University Press, Inc.
Course Instructor: Dr. Eman Azab
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Voltage Comparator
Figure from Sedra/Smith Copyright Β© 2010 by Oxford University Press, Inc.
Positive Feedback is employed
The output voltage is either the high or the low voltagesupply
π£π < π£+ π£π = ππΆπΆ
π£π > π£+ π£π = πππ
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage Logarithmic Amplifier Non-linear logarithmic Amplifier
BJT operates in the Active Region
πππ’π‘ = βππ΅πΈ = βπππππΌπΆπΌπ
πΌπΆ =ππππ 1
πππ’π‘ = βππ΅πΈ = βππππππππΌππ 1
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Voltage anti-Logarithmic Amplifier
Non-linear Anti-logarithmic Amplifier
BJT operates in the Active Region
πππ = βππ΅πΈ = βπππππΌπΆπΌπ
πΌπΆ =πππ’π‘π 1
πππ’π‘ = πΌππ 1expβπππππ
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
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Voltage Multiplier or Divider
πππ’π‘ = πΌππ 1expβπππππ
πππ’π‘ = βππ΅πΈ = βππππππππΌππ 1
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Example
For the 4127 IC showed in figure, find the output voltage (Vout) as a function in the input currents (Ix and Iy).
Using the 4127 IC and the linear/nonlinear op-amp applications, design the following functions with minimum number of op-amps and derive K, n and m as a function in the circuit parameters.
Note that: Q1 and Q2 are matched and Ξ² is large.
πππ’π‘ = πΎπΌπ₯πΌπ¦
π
πππ’π‘ = πΎπΌπ₯πΌπ¦
πβπ
Course Instructor: Dr. Eman Azab
Contact: [email protected]
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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Example Solution
For the 4127 IC showed in figure, find the output voltage (Vout) as a function in the input currents (Ix and Iy).
Note that: Q1 and Q2 are matched and Ξ² is large.
Electronic Circuits for Mechatronics ELCT 609
Summer R2 2020
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