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Lecture 20: Frequency Response: Miller Effect

Lecture 20: Frequency Response: Miller Effect. Prof. Niknejad. Lecture Outline. Frequency response of the CE as voltage amp The Miller approximation Frequency Response of Voltage Buffer. Last Time: CE Amp with Current Input. Can be MOS. Calculate the short circuit current gain of device

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Lecture 20: Frequency Response: Miller Effect

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  1. Lecture 20:Frequency Response: Miller Effect Prof. Niknejad

  2. Lecture Outline • Frequency response of the CE as voltage amp • The Miller approximation • Frequency Response of Voltage Buffer University of California, Berkeley

  3. Last Time: CE Amp with Current Input Can be MOS Calculate the short circuit current gain of device (BJT or MOS) University of California, Berkeley

  4. CS Short-Circuit Current Gain MOS Case MOS BJT 0 dB Note: Zero occurs when all of “gm” current flows into Cgd: University of California, Berkeley

  5. Common-Emitter Voltage Amplifier Small-signal model: omit Ccs to avoid complicated analysis Can solve problem directly by phasor analysis or using 2-port models of transistor OK if circuit is “small” (1-2 nodes) University of California, Berkeley

  6. CE Voltage Amp Small-Signal Model Two Nodes! Easy Same circuit works for CS with University of California, Berkeley

  7. Frequency Response KCL at input and output nodes; analysis is made complicated due to Z branch  see H&S pp. 639-640. Zero Low-frequency gain: Two Poles  Note: Zero occurs due to feed-forward current cancellation as before Zero: University of California, Berkeley

  8. Exact Poles Usually >> 1 These poles are calculated after doing some algebraic manipulations on the circuit. It’s hard to get any intuition from the above expressions. University of California, Berkeley

  9. Miller Approximation Results of complete analysis: not exact and little insight Look at how Z affects the transfer function: find Zin University of California, Berkeley

  10. Input Impedance Zin(j) At output node: Why? University of California, Berkeley

  11. Cx + ─ + ─ AV,Cx AV,Cx + ─ + ─ Vin (1-Av,Cx)Cx Vout Vout (1-1/Av,Cx)Cx Miller Capacitance CM Effective input capacitance: University of California, Berkeley

  12. Some Examples Common emitter/source amplifier: Negative, large number (-100) Miller Multiplied Cap has Detrimental Impact on bandwidth Common collector/drain amplifier: Slightly less than 1 “Bootstrapped” cap has negligible impact on bandwidth! University of California, Berkeley

  13. CE Amplifier using Miller Approx. Use Miller to transform C Analysis is straightforward now … single pole! University of California, Berkeley

  14. Comparison with “Exact Analysis” Miller result (calculate RC time constant of input pole): Exact result: University of California, Berkeley

  15. Method of Open Circuit Time Constants • This is a technique to find the dominant pole of a circuit (only valid if there really is a dominant pole!) • For each capacitor in the circuit you calculate an equivalent resistor “seen” by capacitor and form the time constant τi=RiCi • The dominant pole then is the sum of these time constants in the circuit University of California, Berkeley

  16. Equivalent Resistance “Seen” by Capacitor • For each “small” capacitor in the circuit: • Open-circuit all other “small” capacitors • Short circuit all “big” capacitors • Turn off all independent sources • Replace cap under question with current or voltage source • Find equivalent input impedance seen by cap • Form RC time constant • This procedure is best illustrated with an example… University of California, Berkeley

  17. Example Calculation • Consider the input capacitance • Open all other “small” caps (get rid of output cap) • Turn off all independent sources • Insert a current source in place of cap and find impedance seen by source University of California, Berkeley

  18. Common-Collector Amplifier • Procedure: • Small-signal two-port model • Add device (andother) capacitors University of California, Berkeley

  19. Two-Port CC Model with Capacitors Gain ~ 1 Find Miller capacitor for C -- note that the base-emitter capacitor is between the input and output University of California, Berkeley

  20. Voltage Gain AvC Across C Note: this voltage gain is neither the two-port gain nor the “loaded” voltage gain University of California, Berkeley

  21. Bandwidth of CC Amplifier Input low-pass filter’s –3 dB frequency: Substitute favorable values of RS, RL: Model not valid at these high frequencies University of California, Berkeley

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