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1 Amin Arbabian Jan M. Rabaey Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction Sept. 9 th , 2010 2 Announcements HW2 Posted, due Thurs. Sept. 16 th , 330pm before class in EE142 drop box

Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Page 1: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Amin ArbabianJan M. Rabaey

Lecture 5:Resonance Two-Ports

EE142 – Fall 2010Introduction

Sept. 9th, 2010

2

Announcements

HW2 Posted, due Thurs. Sept. 16th, 330pm before class in EE142 drop box

Page 2: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Overview

Last Lecture– Resonance circuits, series RLC “Tank”

– Passive amplification

– Quality factor

This Lecture– More on Resonant circuits

– Bandwidth of tuned circuits

– Tuned amplifiers

– Introduction to two ports

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Source of Resonance

What makes the circuit resonate?– Reactive components cancel

1

+ + --vL vC

Page 3: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Back to Transfer Function

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Canonical Form

Page 4: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Root Locus

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Selectivity

Page 5: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Selectivity

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Bandwidth and Q

Page 6: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Parallel RLC Circuit

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Circuit Duality

Page 7: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Duality

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Circuit Duality

Basic Circuit Theory, Desoer and Kuh

Page 8: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Q and Phase Response

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Phase Response

Page 9: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Transfer Function

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Parallel RLC Transfer Function

Page 10: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Parallel Resonance

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Tuned Amplifier

Parallel RLC load results in a tuned amplifier. – The impedance of the load

is selective.

How is gain related to Q?

Page 11: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Series-Shunt Transformation

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Transformer

Page 12: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Tank Dominated by Inductor Q

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Inductance Value for Tuned Amplifier

Page 13: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Other Advantages of Tuned Amplifier

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Cascode Tuned Amplifier

Page 14: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Tuned Amplifier Bandwidth

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What are the Limits?

To win some of the bandwidth back requires other techniques, such as shunt peaking and distributed amplifiers. Other techniques (some invented here at Berkeley) can also help out.

But can we tune out parasitics and design amplifiers operating at arbitrarily high frequency?

Based on the simple analysis thus far, it seems that for any given frequency, no matter how high, we can simply absorb the parasitic capacitance of the amplifier with an appropriately small inductor (say a short section of transmission line) and thus realize an amplifier at an arbitrary frequency. This is of course ludicrous and we’ll re-examine this question in future lecture.

Page 15: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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TWO PORT NETWORKS

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Introduction to Two Port Networks

Design problems often need abstraction– Concerned with external behavior (@ “Terminals”)

– A Black-Box view of the component

– Replace by characteristic parameters

When physical circuit models start to fail– High frequency operation

Page 16: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Introduction (2)

A port is defined as a terminal pair where the current entering one terminal is equal and opposite to the current exiting the second terminal.

Any circuit with four terminals can be analyzed as a two-port if it is free of independent sources and the current condition is met at each terminal pair.

All the complexity of the two-port is captured by four complex numbers (which are in general frequency dependent).

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Two Port Network Representations

Various equivalentways of relating the terminal parameters

Page 17: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Conversion Table

W.S.Harwin, University of Reading

All matrices in the same row are equivalent

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Example: Transformer

Page 18: Lecture 5: Resonance Two-Ports - University of California ...bwrcs.eecs.berkeley.edu/.../Lectures/Lect5_2up.pdf · Lecture 5: Resonance Two-Ports EE142 – Fall 2010 Introduction

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Coupled Inductors

Z Matrix