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Emitter-Follower (EF)  Amplifier ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ch. 7 Frequency Response  Part 4 High and Low Frequency AC Equivalent Circuit
EF  Amplifier  -  DC Analysis  (Nearly  the  Same  as  CE  Amplifier) ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ch. 7 Frequency Response  Part 4 R 1  = 10K R 2  = 2.5K R C  = 0 K R E  = 0.33K Note:  Only  difference  here  from  CE  case  is  V CE   is  larger  since  R C  was  left  out  here  in  EF  amplifier.
EF  Amplifier  - Midband  Gain  Analysis Ch. 7 Frequency Response  Part 4 Equivalent  input  resistance R i V i + _ R i V b + _ I π DC analysis is nearly the same! I B  , I C  and g m  are all the same.  Only V CE  is different since R C =0.  V O NOTE:  Voltage gain is only ~1! This is a characteristic of the EF amplifier! Cannot get voltage gain >1 for this amplifier!
Analysis  of  Low  Frequency  Poles  Gray-Searle  (Short  Circuit)  Technique ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ch. 7 Frequency Response  Part 4
Emitter  Follower  - Analysis  of  Low  Frequency  Poles   Gray-Searle  (Short  Circuit)  Technique Ch. 7 Frequency Response  Part 4 Input coupling capacitor C C1  = 2  μ F R i V i I π I X
Emitter  Follower  - Analysis  of  Low  Frequency  Poles   Gray-Searle  (Short  Circuit)  Technique Ch. 7 Frequency Response  Part 4 ,[object Object],[object Object],I π V e I e I X r e So dominant low frequency pole is due to C C1  !
Emitter  Follower - Low  Frequency  Zeros Ch. 7 Frequency Response  Part 4 ,[object Object],[object Object]
Emitter  Follower - Low  Frequency  Poles  and  Zeros Magnitude  Bode  Plot Ch. 7 Frequency Response  Part 4
Emitter  Follower - Low  Frequency  Poles  and  Zeros Phase  Shift  Bode  Plot Ch. 7 Frequency Response  Part 4
Analysis  of  High  Frequency  Poles  Gray-Searle  (Open  Circuit)  Technique ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ch. 7 Frequency Response  Part 4
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 ,[object Object],I e Z eq E I e z π  =1/y π
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 Modified  Equivalent  Circuit Replace  this with  this. Z B ’ Z B ’ z π  =1/y π   Looks  like  a  resistor  in  parallel  with  a  capacitor.
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 R xC π ,[object Object]
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 ,[object Object]
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 ,[object Object],E I e V x I x I π I x -I π I e +g m V π We get the same result here for the high frequency pole associated  with  C π   as we did using the equivalent circuit transformation.
Emitter  Follower - Analysis  of  High  Frequency  Poles   Gray-Searle  (Open  Circuit)  Technique Ch. 7 Frequency Response  Part 4 ,[object Object],V x I x I π I x -I π I π +g m V π E We get the same result here for the high frequency pole associated  with  C µ   as we did using the equivalent circuit transformation.
Emitter  Follower - High  Frequency  Zeros Ch. 7 Frequency Response  Part 4 ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Emitter  Follower - High  Frequency  Poles  and  Zeros Magnitude Ch. 7 Frequency Response  Part 4
Emitter  Follower - High  Frequency  Poles  and  Zeros Phase  Shift Ch. 7 Frequency Response  Part 4
Comparison  of  EF  to  CE  Amplifier  (For R S  = 5 Ω  ) Ch. 7 Frequency Response  Part 4 CE   EF Midband  Gain Low  Frequency  Poles and Zeros High Frequency  Poles and Zeroes Better  low  frequency  response ! Much  better  high  frequency  response !
Conclusions ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ch. 7 Frequency Response  Part 4

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Chap7part4 (2)

  • 1.
  • 2.
  • 3. EF Amplifier - Midband Gain Analysis Ch. 7 Frequency Response Part 4 Equivalent input resistance R i V i + _ R i V b + _ I π DC analysis is nearly the same! I B , I C and g m are all the same. Only V CE is different since R C =0. V O NOTE: Voltage gain is only ~1! This is a characteristic of the EF amplifier! Cannot get voltage gain >1 for this amplifier!
  • 4.
  • 5. Emitter Follower - Analysis of Low Frequency Poles Gray-Searle (Short Circuit) Technique Ch. 7 Frequency Response Part 4 Input coupling capacitor C C1 = 2 μ F R i V i I π I X
  • 6.
  • 7.
  • 8. Emitter Follower - Low Frequency Poles and Zeros Magnitude Bode Plot Ch. 7 Frequency Response Part 4
  • 9. Emitter Follower - Low Frequency Poles and Zeros Phase Shift Bode Plot Ch. 7 Frequency Response Part 4
  • 10.
  • 11.
  • 12. Emitter Follower - Analysis of High Frequency Poles Gray-Searle (Open Circuit) Technique Ch. 7 Frequency Response Part 4 Modified Equivalent Circuit Replace this with this. Z B ’ Z B ’ z π =1/y π Looks like a resistor in parallel with a capacitor.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17.
  • 18. Emitter Follower - High Frequency Poles and Zeros Magnitude Ch. 7 Frequency Response Part 4
  • 19. Emitter Follower - High Frequency Poles and Zeros Phase Shift Ch. 7 Frequency Response Part 4
  • 20. Comparison of EF to CE Amplifier (For R S = 5 Ω ) Ch. 7 Frequency Response Part 4 CE EF Midband Gain Low Frequency Poles and Zeros High Frequency Poles and Zeroes Better low frequency response ! Much better high frequency response !
  • 21.