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4/23/2010 1 EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING Tai-Chang Chen University of Washington, Bothell Spring 2010 EE215 1 WEEK 5 CIRCUIT ANALYSIS (III) & OPERATIONAL AMPLIFIERS April 30 th , 2010 EE215 2 © TC Chen UWB 2010

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  • 4/23/2010

    1

    EE215 – FUNDAMENTALS OF ELECTRICAL ENGINEERING

    Tai-Chang Chen

    University of Washington, Bothell

    Spring 2010

    EE215 1

    WEEK 5CIRCUIT ANALYSIS (III) &

    OPERATIONAL AMPLIFIERS

    April 30th , 2010

    EE215 2© TC Chen UWB 2010

  • 4/23/2010

    2

    QUESTIONS TO ANSWER• Thévenin and Norton Equivalents

    – What are the Thevenin and Northon equivalents?

    – How to simplify electric circuits to those equivalents?

    • Maximum Power Calculation

    – What is the condition of a resistive network to deliver maximum power?

    – How to calculate the maximum power delivered by the network?

    • Operational Amplifier

    – What is an op amp and its circuit symbol?

    – What are the common configurations of op amps and their gains?

    EE215 3© TC Chen UWB 2010

    THÉVENIN AND NORTON EQUIVALENTS

    April 30th , 2010

    EE215 4© TC Chen UWB 2010

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    THÉVENIN AND NORTON EQUIVALENTS

    • Every network consisting of independent and dependent sources and resistors with two terminals a and b can be replaced with equivalent circuits of the following form:

    EE215 5© TC Chen UWB 2010

    THÉVENIN AND NORTON EQUIVALENTS

    • Thévenin and Norton equivalents are very useful if we are only interested in the effect on a load.

    – Example: home power outlet, car battery, …

    • How do we determine vTh and RTh?

    – Open circuit

    – Short circuit

    – Dead network resistance

    EE215 6© TC Chen UWB 2010

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    THÉVENIN AND NORTON EQUIVALENTS

    • Therefore, we know the Thévenin equivalent if we know the open circuit voltage, the short circuit current, or dead network resistance.

    – Don’t try this at home!

    EE215 7© TC Chen UWB 2010

    EXAMPLE (1)

    • Open circuit:

    EE215 8© TC Chen UWB 2010

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    EXAMPLE (1)

    • Short circuit:

    +–

    25V 20

    5 4

    3A

    a

    b

    v0

    EE215 9© TC Chen UWB 2010

    EXAMPLE (2A)

    • We could have obtained the same result with source transformations

    +–

    25V 20

    5 4

    3A

    a

    b

    EE215 10© TC Chen UWB 2010

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    EXAMPLE (2B)

    Replace combined current source with Théveninequivalent:

    5A 205

    4

    3A

    a

    b

    +–

    32V

    8a

    b

    EE215 11© TC Chen UWB 2010

    EXAMPLE (2C)

    EE215 12© TC Chen UWB 2010

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    MAXIMUM POWER TRANSFER

    April 30th , 2010

    EE215 13© TC Chen UWB 2010

    MAXIMUM POWER TRANSFER (1)

    • For what output load RL is the power maximized?

    • General resistive network:

    • Find Thévenin equivalent:+–

    i RLVTh

    RTh a

    b

    i RL

    a

    b

    Resistive network

    EE215 14© TC Chen UWB 2010

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    MAXIMUM POWER TRANSFER (2)

    • Calculate output power p:

    • Find load RL such that p is maximized:

    • Max. power if load is equal to Thévenin resistance

    EE215 15© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER

    April 30th , 2010

    EE215 16© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (1)

    • The operational amplifier, or op amp for short, is a fundamental building block in circuit design. Stuffed inside a chip are a bunch of transistors and other elements that make up a near-ideal voltage controlled voltage source (VCVS) with near-infinite gain. Of course, we'll start by assuming it is ideal…

    EE215 17© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER (2)

    • Circuit Symbol:

    – The op amp has a special circuit symbol, a triangle with two inputs and one output

    EE215 18© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (3)

    • Voltage transfer characteristic: vp

    vn

    +

    V+

    V –

    vo

    in

    ip io

    EE215 19© TC Chen UWB 2010

    • Slew Rate:– At this point we should probably note that another

    departure from ideality in the op amp is that the slew rate, is also limited. This affects how fast the op amp responds to a step change in input, and how high a frequency it can operate at.

    OPERATIONAL AMPLIFIER (4)

    EE215 20© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (5)

    • Operation in the linear region:–

    –•

    • Op amps have very high input resistance.–

    EE215 21© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER (6)

    • Ideal Op Amps Relationships:– An ideal op amp is an ideal voltage controlled voltage

    source. We can think of the op amp symbol being replaced as follows:

    EE215 22© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (7)

    • Negative feedback can be used to ensure operation in the linear region.

    EE215 23© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER (8)

    • Inverting Amplifier:

    EE215 24© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (9)

    • Summing Amplifier:

    EE215 25© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER (10)

    • Non-inverting Amplifier:

    EE215 26© TC Chen UWB 2010

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    OPERATIONAL AMPLIFIER (11)

    • Differential Amplifier:

    EE215 27© TC Chen UWB 2010

    OPERATIONAL AMPLIFIER (12)

    Remember:

    • Input current: ip = in = 0

    • Virtual short condition (in linear region): vp = vn

    • First assume op amp operates in linear region.– If this leads to a contradiction, then op amp is in

    saturation.

    EE215 28© TC Chen UWB 2010