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Physics 2415 Lecture 24: Circuits with AC Source
Physics 2415 Lecture 24: Circuits with AC Source

... Pure Inductance L If we put an alternating voltage across an inductor L, having zero resistance R, this external voltage must be exactly matched by the back emf generated. ...
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... to limit the signal amplitude across each base-emitter junction to a maximum of 5 millivolts. yet another design requirement is that the differential input resistance be at least 100 k. The BJTs that are used in this differential amplifier have a  = 100 (how convenient!). Give the circuit configur ...
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... b) Use the function generator to provide a 10 Vpp sinewave to the input of the double T. Measure the transfer function (Vout vs frequency) between 20Hz and 20kHz. Use more detailed sampling in places where the function changes rapidly. Find values of f0, f1 and f2 (as in figure 2). Use an oscillosco ...
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< 1 ... 819 820 821 822 823 824 825 826 827 ... 984 >

Current mirror

A current mirror is a circuit designed to copy a current through one active device by controlling the current in another active device of a circuit, keeping the output current constant regardless of loading. The current being 'copied' can be, and sometimes is, a varying signal current. Conceptually, an ideal current mirror is simply an ideal inverting current amplifier that reverses the current direction as well or it is a current-controlled current source (CCCS). The current mirror is used to provide bias currents and active loads to circuits. It can also be used to model a more realistic current source (since ideal current sources don't exist).The circuit topology covered here is one that appears in many monolithic ICs. It is a Widlar mirror without an emitter degeneration resistor in the follower (output) transistor. This topology can only be done in an IC as the matching has to be extremely close and cannot be achieved with discretes.Another topology is the Wilson mirror. The Wilson mirror solves the Early effect voltage problem in his design.
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