Notes Integrators& Differentiators

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    Integrators & Differentiators

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    Integrators

    Op Amp RC circuits now

    Opens door to a wide range of useful andexciting applications

    Integrators and Differentiators are twobasic applications

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    Inverting Integrator

    Replacing resistors with generalimpedances

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    Z 2 (s)= 1/Y 2 (s )

    or

    Finite dc Gain is given as

    Which is the T.F of a low passSTC network

    3-dB frequency is

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    The capacitor behaves as open circuit at

    dc , so by inspection the dc gain is simply-R 2 /R 1

    Due to the virtual ground at the invertingterminal the resistance seen by thecapacitor is simply R 2 , hence the timeconstant of the low pass STC network isC 2 R 2

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    =

    Output voltage is proportional tothe time integral of input voltage

    and CR is the integrator TimeConstant.

    Negative sign indicates that it is anInverting Integrator (also known asMiller Integrator).

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    Bode Plot For The Inverting Integrator

    As doubles, the gain is halved (decreases by 6 dB) Intercepts the 0 dB line at =1/RC making gainequal to unity

    This is known as IntegratorFrequency

    Behaves as a low pass STCnetwork with a corner frequency ofzero

    At =0, the T.F becomes infiniteas the capacitor is opened and opamp is operating with open loop

    Any tiny dc component in theinput will saturate the output whichis a serious problem with integratorcircuit

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    Effect of Input Offset DC voltage and current

    R added in the positive lead tokeep the input bias current I B fromflowing through C

    Nevertheless I OS flows through C

    and causes the op amp output tosaturate.

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    Alleviation of dc problem The dc problem can be alleviated by connecting a

    resistor R F across the integrator capacitor C It provides a dc path for the dc currents V OS /R and I OS

    Now v 0 will have a dc component

    instead of rising linearly To keep the dc offset low, one would lower R F

    Lower the value of R F , less ideal the integrator circuit

    becomes

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    Inclusion of R F moves the pole at =0 to =1/CR F and the new T.F becomes

    Lower the value of R F , higher the cornerfrequency will be and more non-ideal the

    integrator becomes Selection of R F , a trade off between dc performance and signal performance

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    The Op Amp Differentiator

    Interchanging the positions of R and C inan ideal Integrator results in Differentiatorcircuit

    Performs the mathematical operation ofsignal differentiation

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    Bode Plot shows that the magnitude doublesfor an octave increase in frequency

    Plot is a straight line of slope 6dB/octaveintersecting the 0 dB line at =1/CR (theDifferentiator Time Constant)

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    The Frequency response of Differentiator can bethought of a High pass STC network with cornerfrequency at infinity

    Differentiator circuit can act as a Noise Magnifieras a spike appears at the output every timethere is a sharp change at the input

    This causes stability problems, so they are

    generally avoided Sometime a small-valued resistor is used inseries with the capacitor, but it introduces non-ideal behavior to the circuit