dr. eman azab microelectronics elct 703 (w19) lecture 1

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MICROELECTRONICS ELCT 703 (W19) LECTURE 1: ANALOG MULTIPLIERS Dr. Eman Azab Assistant Professor Office: C3.315 E-mail: [email protected] DR. EMAN AZAB ELECTRONICS DEPT., FACULTY OF IET THE GERMAN UNIVERSITY IN CAIRO 1

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Page 1: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

MICROELECTRONICS ELCT 703 (W19) LECTURE 1: ANALOG MULTIPLIERS

Dr. Eman Azab

Assistant Professor

Office: C3.315

E-mail:

[email protected]. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

1

Page 2: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

COURSE OVERVIEWCourse Team

Lecturer

Dr. Eman AzabE-mail: [email protected]

Office: C3.315

Office hours: Via E-mail

Teaching

Assistant

Eng.: Radwa KhairyE-mail: [email protected]

Office: C3.307

Office hours: Via E-mail

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

2

Teaching Method Location

One Lecture per Week

(Thursday 2nd Slot)H6

One Tutorial per Week

(Tuesday 1st/3rd)

Check Your

Schedule

Evaluation Method Percentage %

Assignments 10

Quizzes 15

Project 10

Mid-Term 25

Final 40

Page 3: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

COURSE GUIDELINES Please follow GUC regulations for attendance

Course Prerequisites:

Semiconductors

Electronic Circuits

Radio Frequency

Course Objectives: Analog Signal Processing Circuits Design

Analog Multipliers: Differential Amplifier

Op-amp Circuit design, non-idealities, Linear and Non-linear applications

Active RC Filters

Switched capacitor circuits and applications

Operational Trans-conductance Amplifiers Circuit design and Applications

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

3

Page 4: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

TENTATIVE COURSE SCHEDULELecture # Lecture Description

1Revision: Differential Amplifiers & Analog

MultipliersAnalog Multipliers Transistor level design

2 &3 Feedback and Power Amplifiers Feedback Theory in Electronic Circuits and Power amplifiers

4 & 5 Op-amp Circuit design & non-idealities Op-amp Circuit design on the transistor level & Non-ideal

characteristics of Op-amp Circuit realization

6 Compensation TheoryCompensation theory: How to design Stable closed loop systems

using Op-amp?

7 & 8 Op-amp Circuit Applications Linear and Non-linear Closed-loop Applications using Op-amps

9 Active-RC Filters Op-amp based Filters

10 & 11 Switched Capacitors Circuits SC Circuits Design Concept and Applications

12Operational Trans-conductance Amplifiers

Circuit design & ApplicationsOTA CMOS Transistor Level Circuit Design

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

4

Page 5: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

TENTATIVE COURSE EVALUATION SCHEDULE

Assignment Quiz Project

Milestone 1: CMOS Op-

amp Modeling (Verilog A)

Quiz 1: Feedback and

Compensation Theory

Milestone 2: CMOS Op-

amp Circuit Design

(Simulation)

Milestone 3: Op-amp

Application (Simulation)

Assignment 1: Feedback and

Compensation Theory

Mid-Term

Milestone 4: PCB for Op-

amp Application

(Hardware)

Assignment 2: Research Paper

Part 1

Quiz 2: Op-amp

nonlinear Applications

Assignment 3: Research Paper

Part 2

Quiz 3: OTA-C/Switched

cap Filters

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

5

Page 6: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

COURSE GRADING RULES

Grading scheme is based on GUC Regulations

Copies will be graded as ZERO

This is applicable for Assignments, quizzes and Projects

Stick to the office hours for questions

Send an e-mail for urgent questions

Attend the lectures and take notes!

All the Course material will be available on the website

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

6

Page 7: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

REFERENCES1. β€œAnalysis and Design of Analog Integrated Circuits”, Gray,

Hurst, Lewis & Meyer

2. β€œ Fundamentals of Microelectronics”, Razavi

3. β€œ Design of Analog CMOS Integrated Circuits”, Razavi

4. β€œAnalog Integrated Circuit Design”, Johns & Martin

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

7

Page 8: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIERS Transistor level Circuit

Design

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

8

Page 9: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIERS: INTRODUCTIONAnalog Multiplier is a circuit that takes two analog inputs (I/V) andgenerate an output proportional to their Product

K is the multiplication gain factor

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

9

π‘‹π‘œπ‘’π‘‘ = 𝐾 𝑋𝑖1 Γ— 𝑋𝑖2

Multiplier

(K)

Xi1

Xi2

Xout

Page 10: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

10

Amplitude Modulation Illustration

The circuit is used in communication systems for modulation/demodulation

Page 11: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

11

Analog Multipliers can be one, two or four quadrant multipliers

This classification depends on the polarity of the input signals

Multiplier

(K)

Xi1

Xi2

Xout

Multiplier Xi1 Xi2

Single (one) Quadrant Unipolar Unipolar

Two Quadrant Unipolar Bipolar

Four Quadrant Bipolar Bipolar

Page 12: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

Emitter Coupled Circuit can beused as a two Quadrant analogmultiplier

It is formed with two matchedBJT with their emitters connectedtogether

Assume Q1 and Q2 are Active and Ξ²F

is large

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

12

𝐼𝐸1 + 𝐼𝐸2 = 𝐼

𝐼𝐢1 = 𝐼𝑠𝑒𝑉𝐡𝐸1𝑉𝑇 𝐼𝐢2 = 𝐼𝑠𝑒

𝑉𝐡𝐸2𝑉𝑇

𝐼𝐢1 β‰… 𝐼𝐸1 & 𝐼𝐢2 β‰… 𝐼𝐸2

Where Is is the reverse saturation current and VT is the thermal voltage

(25mV @ room temperature)

Page 13: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

The input voltage Vi1 changesthe collector currents

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

13

𝑉𝑖1 = 𝑉𝐡𝐸1 βˆ’ 𝑉𝐡𝐸2𝐼𝐢2𝐼𝐢1

= π‘’βˆ’π‘‰π‘–1𝑉𝑇

𝐼𝐢1 + 𝐼𝐢2 = 𝐼𝐢1 + 𝐼𝐢1π‘’βˆ’π‘‰π‘–1𝑉𝑇 β‰… 𝐼

𝐼𝐢1 =𝐼

1 + π‘’βˆ’π‘‰π‘–1𝑉𝑇

𝐼𝐢2 =𝐼

1 + 𝑒𝑉𝑖1𝑉𝑇

Page 14: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

The ECC differential output current orvoltage is related to the input voltageβ€œVi1” and biasing current β€œI” as follows:(Prove that:)

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

14

βˆ†πΌπΆ = 𝐼𝐢1 βˆ’ 𝐼𝐢2

βˆ†πΌπΆ = 𝐼 tanh𝑉𝑖12𝑉𝑇

βˆ†π‘‰πΆ = βˆ’πΌπ‘…πΆ tanh𝑉𝑖12𝑉𝑇

βˆ†π‘‰πΆ = 𝑉𝐢1 βˆ’ 𝑉𝐢2

Note: tanh(x) β‰ˆ x for x<<1

Page 15: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

To use ECC as a multiplier, the followingcondition must be satisfied:

The input voltage Vi1 value must be lessthan 50mV (2VT)

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

15

Note: tanh(x) β‰ˆ x for x<<1

for Vi1<<2VT

βˆ†π‘‰πΆ β‰… βˆ’π‘…πΆ2𝑉𝑇

𝐼 𝑉𝑖1

βˆ†πΌπΆ β‰…1

2𝑉𝑇𝐼 𝑉𝑖1βˆ†πΌπΆ = 𝐼 tanh

𝑉𝑖12𝑉𝑇

βˆ†π‘‰πΆ = βˆ’πΌπ‘…πΆ tanh𝑉𝑖12𝑉𝑇

Page 16: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

The ECC output is proportional to themultiplication of the differential inputvoltage β€œVi1” and the biasing current β€œI”

ECC is a two quadrant multiplier as thecurrent β€œI” is unipolar

If the current β€œI” becomes negative, Q1 and Q2will not operate in the active mode, then theexponential equation is not valid anymore

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

16

for Vi1<<2VT

βˆ†π‘‰πΆ β‰… βˆ’π‘…πΆ2𝑉𝑇

𝐼 𝑉𝑖1βˆ†πΌπΆ β‰…1

2𝑉𝑇𝐼 𝑉𝑖1

𝐾𝑉 = βˆ’π‘…πΆ2𝑉𝑇

𝐾𝐼 =1

2𝑉𝑇 Note: tanh(x) β‰ˆ x for x<<1

Page 17: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: EMITTER COUPLED CIRCUIT

The ECC can be modified to be a twoquadrant voltage multiplier by replacingthe biasing current source β€œI” with thecircuit shown

The circuit has another condition on β€œVi2”to work as a multiplier

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

17

for Vi1<<2VT

𝐼 =𝑉𝑖2 βˆ’ 𝑉𝐡𝐸,π‘œπ‘›

𝑅

βˆ†π‘‰πΆ β‰… βˆ’π‘…πΆ2𝑉𝑇

𝑉𝑖2 βˆ’ 𝑉𝐡𝐸,π‘œπ‘›π‘…

𝑉𝑖1

for Vi1<<2VT & Vi2>>VBE,on

βˆ†π‘‰πΆ β‰… βˆ’π‘…πΆ2𝑉𝑇𝑅

𝑉𝑖2𝑉𝑖1 𝐾𝑉 = βˆ’π‘…πΆ2𝑅𝑉𝑇

Figure from Gray & Mayer, β€œAnalysis and Design of Analog Integrated Circuits”

John Wiley & Sons, inc.

Page 18: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

The ECC is used as a basicbuilding unit for a four quadrantmultiplier: Gilbert Cell

The circuit is formed with threecross coupled ECCs as shown inFigure

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

18

βˆ†πΌπΆ = 𝐼𝐢3βˆ’5 βˆ’ 𝐼𝐢4βˆ’6

βˆ†πΌπΆ = 𝐼𝐢3 + 𝐼𝐢5 βˆ’ 𝐼𝐢4 + 𝐼𝐢6

βˆ†πΌπΆ = 𝐼𝐢3 βˆ’ 𝐼𝐢4 + 𝐼𝐢5 βˆ’ 𝐼𝐢6

𝐼𝐢3 βˆ’ 𝐼𝐢4 = 𝐼𝐢1 tanh𝑉𝑖12𝑉𝑇

𝐼𝐢5 βˆ’ 𝐼𝐢6 = 𝐼𝐢2 tanh βˆ’π‘‰π‘–12𝑉𝑇

= βˆ’πΌπΆ2 tanh𝑉𝑖12𝑉𝑇

Figure from Gray & Mayer, β€œAnalysis and Design of Analog Integrated Circuits”

John Wiley & Sons, inc.

Page 19: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

Gilbert Cell analysis (Cont.)

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

19

βˆ†πΌπΆ = 𝐼𝐢3 βˆ’ 𝐼𝐢4 + 𝐼𝐢5 βˆ’ 𝐼𝐢6

𝐼𝐢1 βˆ’ 𝐼𝐢2 = 𝐼 tanh𝑉𝑖22𝑉𝑇

βˆ†πΌπΆ = 𝐼𝐢1 βˆ’ 𝐼𝐢2 tanh𝑉𝑖12𝑉𝑇

βˆ†πΌπΆ = 𝐼 tanh𝑉𝑖12𝑉𝑇

tanh𝑉𝑖22𝑉𝑇

for Vi1 & Vi2 <<2VT

βˆ†πΌπΆ ≅𝐼

2𝑉𝑇2𝑉𝑖1𝑉𝑖2 𝐾𝐼 =

𝐼

2𝑉𝑇2

Page 20: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

Gilbert Cell is a four quadrantmultiplier

The differential output current isproportional to the multiplication ofthe voltages β€œVi1” and β€œVi2”

the voltages β€œVi1” and β€œVi2” mustbe less than 50mV (2VT)

The output current can beconverted to a voltage signal

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

20

βˆ†π‘‰πΆ β‰… βˆ’πΌπ‘…πΆ2𝑉𝑇

2𝑉𝑖1𝑉𝑖2 𝐾𝑉 = βˆ’

𝐼𝑅𝐢2𝑉𝑇

2

Page 21: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

To remove the constraint of the input voltage to be less than 50mV, thefollowing Circuit can be used

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

21

𝑉𝑖1β€² ∝ tanhβˆ’1 𝑉𝑖1

𝑉𝑖2β€² ∝ tanhβˆ’1 𝑉𝑖2

βˆ†πΌπΆ = 𝐼 tanh𝑉𝑖1β€²

2𝑉𝑇tanh

𝑉𝑖2β€²

2𝑉𝑇

Page 22: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

To remove the constraint of the inputvoltage to be less than 50mV, thefollowing Circuit can be used

Assume Q7 and Q8 Active and matched withlarge Ξ²

The Differential voltage-to-current Converterhas the output current given as:

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

22Figure from Gray & Mayer, β€œAnalysis and Design of Analog Integrated Circuits”

John Wiley & Sons, inc.

𝑉𝑖1β€² = 𝑉𝐡𝐸8 βˆ’ 𝑉𝐡𝐸7

𝑉𝑖1β€² = 𝑉𝑇𝑙 𝑛

𝐼𝑐8𝐼𝑐7

= 𝑉𝑇𝑙𝑛𝐼2𝐼1

𝐼2 = πΌπ‘œ1 +1

𝑅1𝑉𝑖1 𝐼1 = πΌπ‘œ1 βˆ’

1

𝑅1𝑉𝑖1

Page 23: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

The Differential voltage-to-current Converterhas the output current given as:

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

23

𝑉𝑖1β€² = 𝑉𝑇𝑙 𝑛

𝐼𝑐8𝐼𝑐7

= 𝑉𝑇𝑙𝑛𝐼2𝐼1

𝐼2 = πΌπ‘œ1 +1

𝑅1𝑉𝑖1 𝐼1 = πΌπ‘œ1 βˆ’

1

𝑅1𝑉𝑖1

𝑉𝑖1β€² = 𝑉𝑇𝑙 𝑛

πΌπ‘œ1 +1𝑅1

𝑉𝑖1

πΌπ‘œ1 βˆ’1𝑅1

𝑉𝑖1

= 𝑉𝑇𝑙𝑛1 +

𝑉𝑖1𝑅1πΌπ‘œ1

1 βˆ’π‘‰π‘–1𝑅1πΌπ‘œ1

𝑙 𝑛1 + π‘₯

1 βˆ’ π‘₯= 2 tanhβˆ’1 π‘₯

𝑉𝑖1β€² = 𝑉𝑇𝑙 𝑛

1 +𝑉𝑖1𝑅1πΌπ‘œ1

1 βˆ’π‘‰π‘–1𝑅1πΌπ‘œ1

= 2𝑉𝑇 tanhβˆ’1

𝑉𝑖1𝑅1πΌπ‘œ1

Note that:

Page 24: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

Now the Output differential Current of Gilbert Cell is:

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

24

βˆ†πΌπΆ = 𝐼 tanh𝑉𝑖1β€²

2𝑉𝑇tanh

𝑉𝑖2β€²

2𝑉𝑇

𝑉𝑖1β€² = 2𝑉𝑇 tanh

βˆ’1𝑉𝑖1𝑅1πΌπ‘œ1

𝑉𝑖2β€² = 2𝑉𝑇 tanh

βˆ’1𝑉𝑖2𝑅2πΌπ‘œ2

βˆ†πΌπΆ = 𝐼 tanh2𝑉𝑇 tanh

βˆ’1 𝑉𝑖1𝑅1πΌπ‘œ1

2𝑉𝑇tanh

2𝑉𝑇 tanhβˆ’1 𝑉𝑖2

𝑅2πΌπ‘œ22𝑉𝑇

βˆ†πΌπΆ =𝐼

𝑅1𝑅2πΌπ‘œ1πΌπ‘œ2𝑉𝑖1𝑉𝑖2 𝐾𝐼 =

𝐼

𝑅1𝑅2πΌπ‘œ1πΌπ‘œ2

Page 25: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

Circuit Implementation of Differential voltage to differential CurrentConverter:

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

25

πΌπ‘œ1 =𝑉𝐢𝐢 βˆ’ 𝑉𝐡𝐸13,π‘œπ‘›

𝑅

𝐼1 = πΌπ‘œ1 +𝑉𝑖1𝑅1

𝐼1 = πΌπ‘œ1 βˆ’π‘‰π‘–1𝑅1

Page 26: Dr. Eman Azab MICROELECTRONICS ELCT 703 (W19) LECTURE 1

ANALOG MULTIPLIER: GILBERT CELL

Assignment: Draw the complete Gilbert CellMultiplier (Transistor Level)

DR. EMAN AZAB

ELECTRONICS DEPT., FACULTY OF IET

THE GERMAN UNIVERSITY IN CAIRO

26