Chapter 9 Common Emitter Amplifiers (PowerPoint)

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							            Chapter 9
Common-Emitter Amplifiers
Pictures are redrawn (with some modifications) from
  Introductory Electronic Devices and Circuits
                         By
                  Robert T. Paynter




                                                      1
               Objectives
• Describe AV, AI, AP associated with the three
  amplifier configurations.
• Describe the input/output voltage and current
  phase relationships.
• Calculate the ac emitter resistance of a transistor.
• Discuss two roles of the capacitors in the circuits.
• Derive the ac equivalent circuit for a given
  amplifier.
• Explain how the voltage gain drift due to
  temperature occurs.
• Discuss the relationship between the load
  resistance and voltage gain of a CE amplifier.
                                                         2
        Objectives (Cont.)
• Calculate Zin(base) and Zin for a CE amplifier
• Discuss the effects of swamping on the ac
  characteristics of a CE amplifier
• List and describe the four ac h-parameters




                                                   3
Fig 9.1 Common-emitter input-
        output phase relationship.
    VB
                        +VCC
    IB   15 A
         10 A
          5 A              RC
                 RB

                            Q1

                                 VC   8V
                                      6V
                 Ai = 100             4V
                                 IC   1.5 mA
                                      1 mA
                                      500 A   4
 AC Emitter Resistance

                             25mV
                       re 
                               IE


where r’e = ac emitter resistance
       IE = the dc emitter current, found as VE / RE for
       example.




                                                           5
  Fig 9.2 Example 9.1.
                               R2              2.2kΩ
                  VB  VCC            10V          1.8V
        +10 V                R1  R2          12.2kΩ

                                      VE VB  0.7V
                              IE                  1.1mA
            RC                        RE    1kΩ
  R1
10k        4k
                                      25mV 25mV
                              re                 22.7Ω
                       RL               IE   1.1mA
           hFE = 300   15k
   R2
2.2k       RE
            1k
                                                             6
Fig 9.3 Graphical determination of
        ac emitter resistance.
         IE




   IE                 Q2

                                    VBE
                            re 
              Q1                    I E

   IE
                              VBE
               VBE VBE                   7
  Fig 9.4 The determination of ac beta.
      IC


                  I C ic
            ac      
                  I B ib


                     Q
                                 hFE = dc beta
IC
                                 hfe = ac beta



                            IB
                      IB
                                                 8
      AC Model of A BJT
                             c

                                 ic = acib
      C         C
B         B         b
                        ib
      E         E            r'e
npn       pnp
                             e


                                              9
 Roles of Capacitors in Amplifiers

1. A coupling capacitor passes an ac
   signal from one amplifier to another,
   while providing dc isolation between the
   two.
2. A bypass capacitor is used to “short
   circuit” an ac signal to ground while not
   affecting the dc operation of the circuit.


               1   The higher the freq.,
      XC 
             2 fC the lower the capacitor impedance.
                                                        10
Fig 9.5 Coupling capacitors in a
        multistage amplifer.
                    VCC


                          CC3
     CC1
              CC2
                            Load



                                   11
Fig 9.6a AC coupling.

              GND


                    CC3
CC1
        CC2
                     Load



                            12
Fig 9.6b DC isolation.

              VCC


                    CC3
CC1
        CC2
                     Load



                            13
Fig 9.7 Capacitive vs. direct
            coupling.
        VCC             VCC




   CC




                                14
Fig 9.8-9 Bypass capacitors.
 VCC               GND                  VCC




       CB                     CB                     CB


            For AC analysis        For DC analysis
                                                      15
 Fig 9.10 Typical common-emitter
          amplifier signals.
                       VCC      1.8V
       5.6V
                                       5.6V
1.8V
                                              0V
0V




              1.1VDC   1.1VDC
                                               16
 Fig 9.11 Deriving the CE ac-
          equivalent circuit.


R1   RC                  R1     RC   R1         RC

             RS = 0 
       VCC   (ideally)

R2   RE                  R2     RE   R2         RE




     (a)                      (b)         (c)

                                                     17
Fig 9.12a Example 9.2.
           VCC



                 RC
      R1           CC2

     CC1
             Q1               RL


      R2
                 RE      CB

                                   18
Fig 9.12b Example 9.2.


                GND
           RC
     R1



          Q1          RL


     R2
           RE

                           19
Fig 9.12c-d Example 9.2.

                 Q1    RC      RL
 (c)
       R1   R2




                 Q1   RC||RL
 (d)
       R1||R2

                                    20
         Voltage Gain of CE
              Q1           RC||RL

R1||R2


                          vout      vout  ic  RC RL 
               ic = ib    RC||RL         ic rC where rC  RC RL
vin      ib
              Q1                    vin  ie re
              r'e
                                            vout   ir      r
R1||R2                              Av           c C  C
                                            vin     ie re re
                                                                 21
 Fig 9.13 Example 9.4. (1)
        +20 V          Transform the base circuit to its
                       Thevenin equivalent.
                                                    R2           20kΩ
                                      Vth  VCC            20V
   R1       RC                                    R1  R2       170kΩ
150k       12k                          2.353V
                                      Rth  R1 R2  20kΩ 150kΩ
                          RL              17.65kΩ
           hFE = 200      50k
  R2
            RE                       Vth  VBE          2.353V  0.7V
20k                      IB                      
            2.2k                Rth  (hFE  1) RE 17.65kΩ  201 2.2kΩ
                              3.595μA

                                                                        22
 Fig 9.13 Example 9.4. (2)
        +20 V          I C  hFE I B  200  3.595μA  718.9μA
                       I E   hFE  1 I B  201 3.595μA  722.5μA

                       VCE  VCC  I C RC  I E RE
   R1       RC
                            20V  718.9μA 12kΩ  722.5μA  2.2kΩ
150k       12k
                            9.784V      active 
                       RL         25mV    25mV
                            re                 34.6Ω
           hFE = 200   50k         IE   722.5μA
                                 rC  RC RL  12kΩ 50kΩ  9.677kΩ
  R2
20k        RE                         rC     9.677kΩ
            2.2k             Av                   279.7
                                       re     34.6Ω


                                                                       23
Fig 9.14 Example 9.5. (1)
        +10 V
                    Transform the base circuit to its
                    Thevenin equivalent.
                                                 R2           4.7kΩ
            RC                     Vth  VCC            10V
  R1                                           R1  R2       22.7kΩ
            1.5k
18k                                   2.070V
                                   Rth  R1 R2  4.7kΩ 18kΩ
                        RL
           hFE = 30                    3.727kΩ
           hfe = 200    5k
   R2
4.7k       RE                     Vth  VBE         2.070V  0.7V
                        IB                      
            1.2k              Rth  (hFE  1) RE 3.727kΩ  311.2kΩ
                           33.49μA

                                                                      24
Fig 9.14 Example 9.5. (2)
        +10 V          I C  hFE I B  30  33.49μA  1.005mA
                       I E   hFE  1 I B  31 33.49μA  1.038mA

                       VCE  VCC  I C RC  I E RE
            RC              10V  1.005mA 1.5kΩ  1.038mA  1.2kΩ
  R1        1.5k
18k                        7.247V      active 

           hFE = 30       RL re  25mV  25mV  24.08Ω
                          5k        IE  1.038mA
           hfe = 200              rC  RC RL  1.5kΩ 5kΩ  1.154kΩ
   R2
4.7k       RE                 Av  
                                        rC
                                            
                                               1.154kΩ
                                                        47.91
            1.2k                       re     24.08Ω



                                                                      25
        CE Current Gain
                          iout
                   Ai 
                           iin

Ai is always less than hfe due to two factors:
1.The input ac current is divided between
  the transistor and the biasing network.
2.The output collector current is divided
  between the collector resistor and the
  load.


                                                 26
             Power Gain
                      Ap  Ai Av


Example 9.7 The amplifier shown in Fig. 9.5 has
values of Av = 45.3 and Ai = 20. Determine the
power gain (Ap) of the amplifier and the output
power when Pin = 80 W.

              Ap  AAv  2  4 . 0
                    i     0 53 9 6

          Pot  A P  9 6 8 μ  7 . 8 W
            u     pi
                   n   0 0 W 24 m



                                                  27
    The Effects of Loading

                 RC      RL                         RC     RL
                 3k     12k                       3k    6k


    R1||R2   r'e=25                   R1||R2   r'e=25


    rC  RC RL  2.4kΩ                 rC  RC RL  2kΩ
           rC                                rC
     Av    96                      Av    80
           re                               re

The lower the load resistance is, the lower the voltage gain.
                                                                28
          Example 9.8
The load in Fig. 9.16 is open. Calculate the
open-load voltage gain of the circuit.


                 rC  RC  3kΩ

             rC   3kΩ
       Av          120 (max. gain)
             re  25Ω




                                               29
          Calculating Amp.
          Input Impedance
             VCC
                                Z in  R1 R2 Z in(base)
             R1

                                DC: RIN(base)   hFE  1 RE
                                                 hFE RE
             R2
Zin                 Zin(base)   AC: Z in(base)   h fe  1 re
                                                 h fe re

      Biasing circuit
                                                                   30
             Fig 9.17 Example 9.9.
                            +10 V


                                     RC
               R1                    1.5k
             18k

                                    hFE = 30       RL          Z in(base)  h fe re
                                                   5k
                                    hfe = 200
                                                                           200  24Ω  4.8kΩ
                R2
      Zin             Zin(base)      RE
             4.7k
                                     1.2k                     Zin  R1 R2 Zin(base)
                                                                     18kΩ 4.7kΩ 4.8kΩ
                                      Q1
                                                RC       RL          2.1kΩ
                                                1.5k    5k
        R1       R2
Zin                     Zin(base)
      18k    4.7k
                                      r'e = 24
                                      hfe = 200                                                 31
         Calculating the Value of Ai
                                                                    iout
                                                ic
                                iin        ib
                                                       Q1        RC v            RL
                                                                      out
               vin
                                R1    R2
                         Zin               Zin(base)



      i                    i                                vin  iin Zin  ib Zin(base)
 Ai  out           h fe  c
       iin                 ib                                     ib Zin(base)       ib  h fe  1 re
                                                        iin                    
  vout  ic  RL RC   ic rC  iout RL                             Zin                  Zin
            ic rC                                                        Z in rC
 iout                                                Ai   h fe
             RL                                                       Z in(base) RL
                                                                                                      32
                    Example 9.10
  Calculate the value of Ai for the circuit shown in Fig.
  9.17.

                                                         RC          RL
                                                  Q1
                                                         1.5k       5k
                    R1        R2
            Zin                       Zin(base)
                  18k     4.7k
                                                  r'e = 24
                                                  hfe = 200

                                                            Z in rC
Z in(base)  h fe re  200  24Ω  4.8kΩ     Ai  h fe
                                                         Z in(base) RL
Z in  R1 R2 Z in(base)  2.1kΩ
                                                              2.1kΩ 1.15kΩ
                                                   200 
rC  RC RL  1.15kΩ                                            4.8kΩ  5kΩ
                                                   20.2                     33
               Multistage Amp.
               Gain Calculations
AvT  Av1 Av 2 Av 3     Procedure:

AiT  Ai1 Ai 2 Ai 3     1. Do dc analysis
                        2. Find r’e for each stage
ApT  AvT AiT
                        3. Find rC for each stage
                        4. Using r’e and rC to find Av
                           for each stage

Input impedance of next stage is the load of current stage.
          (Zin of next stage is RL of current stage)
                                                              34
   Fig 9.18 Example 9.11. (1)
                                                           +15V
                       R3                           R7
              R1       5k              R5          5k
       CC1    22k                      15k

                      Q1   CC2                     Q2 CC3             RL
                                                                      10k
              R2       R4               R6         R8
                                 CB1                         CB2 hFE = 150
              3.3k    1k              2.5k      1k
                                                                 hfe = 200


Determine Av of the 1st          The input impedance of the 2nd stage:
stage. Assume that r’e
for the 1st stage is 19.8     Zin(base)   h fe  1 re  20117.4  3.497kΩ
and r’e for the 2nd stage is
found to be 17.4 . For        Z in  R5 R6 Z in ( base )  1.329kΩ
the 2nd stage, hfe is 200.
                                                                                  35
Fig 9.18 Example 9.11. (2)
                                                   +15V
                  R3                         R7
        R1        5k              R5        5k
 CC1    22k                       22k

                 Q1   CC2                  Q2 CC3         RL
                                                          10k
        R2        R4               R6      R8
                            CB1                     CB2 hFE = 150
        3.3k     1k              3.3k   1k
                                                        hfe = 200

             rC  R3 Zin  5kΩ 1.33kΩ=1.05kΩ

 Finally, Av for the 1st stage is found as

                         rC     1.05kΩ
                Av                  53.03
                         re    19.8Ω
                                                                    36
        Example 9.12. (1)
Determine the value of AvT for the amplifier in Figure
9.18.
rC for the 2nd stage can be found as

                      rC  R7 RL  3.33kΩ

Av for the 2nd stage is found as
                     rC   3.33kΩ
               Av             191.38
                     re  17.4Ω

        AvT  Av1 Av 2   53.03 191.38  10.15 103

                                                            37
Fig 9.19 The swamped CE amplifier
         and its ac equivalent ckt.
        +VCC              Swamped amplifier is an
                          amplifier that uses a partially
                          bypassed emitter resistance to
             RC           increase ac emitter resistance.
       R1                 Also referred to as a gain-
  C1                      stabilized amplifier.
            Q1 C2    RL

  R2         rE                               rC
                                        Q1
                            R1//R2
       RE           CB                   rE

                                                            38
          Av of Swamped Amp.
                                rC
                     Q1
                                                   vout    ic rC
                                              Av       
       R1//R2
                      rE                           vin ie  re  rE 

                                                              rC
                                       vout      Av  
                                                          re  rE
                          ic = acib    rC
vin                  Q1
      R1//R2    ib    r'e

                      rE

                                                                         39
Fig 9.20 Example 9.13. (1)
          +10V
                                        R2          4.7kΩ
                          Vth  VCC            10V         2.070V
                                      R1  R2       22.7kΩ
             RC           Rth  R1 R2  18kΩ 4.7kΩ  3.727kΩ
   R1        1.5k
   18k                                               Vth  VBE
                                      IB 
            hFE = 200     RL                 Rth   hFE  1 rE  RE 
            hfe = 150     10k
                                                2.070V  0.7V
   R2        rE                          
   4.7k     300                          3.727kΩ   2011210Ω 
                                           5.550μA
     RE
   910
                     CB               I C  hFE I B  200  5.550μA
                                          1.110mA
                                      I E   hFE  1 I B  201 5.550μA
                                          1.116mA                          40
Fig 9.20 Example 9.13. (2)
         +10V       VCE  VCC  I C RC  I E  rE  RE 
                          10V  1.110mA 1.5kΩ  1.116mA  1210Ω 

            RC            6.985V (active)
  R1        1.5k
  18k                                    25mV     25mV
                                  re                   22.41Ω
           hFE = 200      RL                IE   1.116mA
           hfe = 150      10k
  R2        rE                    rC  RC RL  1.304kΩ
  4.7k     300
                                        rC         1.304kΩ
     RE                    Av                              4.046
   910
                    CB              re  rE    22.41Ω  300Ω


                                                                         41
              Example 9.14
Determine the change in gain for the amplifier in Example
9.13 when r’e doubles in value.

                          rC         1.304kΩ
             Av                              3.782
                      re  rE    44.82Ω  300Ω

                 Av  4.046  3.782  0.2639




    Swamping improves the gain stability of a CE
            amplifier when rE >> r’e.

                                                            42
The Effect of Swamping on Zin
                                              c


                                         b
 Z in(base)   h fe  1 re
                                                   r'e
                                  Zin(base)
            h fe re                             e           c


                                                         b
       Zin(base)   h fe  1  re  rE 
                                                                  r'e
                                                  Zin(base)
                   h fe  re  rE                              e
                                                                  rE
                                                                        43
     Fig 9.22 Gain stabilization.


                                                   rE


                     RE                           RE


Av                        -rC / r’e               -rC / (r’e+rE)

Zin(base)                  hfer’e                  hfe(r’e+rE)

Advantage      Higher values of Av than     Relatively stable Av.
               the swamped amplifier.       Much smaller distortion.
Disadvantage   Relatively unstable values   Lower Av than the
               of Av.                       standard amplifier.
                                                                       44
The Hybrid Equivalent Model

           I1                      I2
 1                                           2
                 Two-Port
      V1          System                V2

 1'                                          2'

Hybrid model is derived from two-port system.


                                                  45
Six Circuit-Parameter Models
    for Two-Port Systems
Independent   Dependent    Circuit Parameters
  Variables    Variables

   I1, I2       V1, V2     Impedance Z

   V1, V2        I1, I2    Admittance Y

   V1, I2       I1, V2     Inverse Hybrid g

   I1, V2       V1, I2     Hybrid h

   V2, I2       V1, I1     Transmission T

                           Inverse Transmission
   V1, I1       V2, I2     T’
                                                  46
Equations for Hybrid Model
             V1  h11I1  h12V2
             I 2  h21I1  h22V2

Let V1 = Vi, I1 = Ii, V2 = Vo, and I2 = Io.
Then
             Vi  h11Ii  h12Vo
             I o  h21Ii  h22Vo

                                              47
          Equivalent Circuit for
             Hybrid Model

          Ii                                           Io
1                                                                2
                  hi
     Vi           hrVo               hfIi      ho           Vo

1'                                                               2'

               Vi  h11I i  h12Vo  hi I i  hrVo
               I o  h21I i  h22Vo  h f I i  hoVo
                                                                      48
           h-Parameters
      Vi                    Vi
h11                  h12 
      Ii   Vo  0           Vo    Ii  0
      Io                     Io
h21                   h22 
      Ii   Vo  0            Vo   Ii  0

h11 = hi = Input Resistance
h12 = hr = Reverse Transfer Voltage Ratio
h21 = hf = Forward Transfer Current Ratio
h22 = ho = Output Admittance
                                            49
    h-Parameters for CE Amp.
•   hie = the base input impedance
•   hfe = the base-to-collector current gain
•   hoe = the output admittance
•   hre = the reverse voltage feedback ratio



              vbe  hieib  hre vce
               ic  h feib  hoe vce

                                               50
                      Hybrid Model for
                      CE Configuration
                                   ib                                     ic
                               b                                               c
                      ic                 hie
        ib                 c                               hfeib   hoe
b                                        hrevce

                 ie                vbe                                   vce
                                                      ie
             e
                                                  e
          vin                                  ic
    hie      (output shorted)           hoe      (input open)
          ib                                   vce                  May be
                                                                    neglected.
           ic                                  vbe
    h fe     (output shorted)           hre      (input open)
           ib                                  vce
                                                                                   51
h-parameters of 2N3904




                         52
Hybrid Model without hre and hoe
b                                          c
        ib                      ic
              hie              hfeib               h fe   ac

                                                   hie   hfe  1 re  hfe re  Z in(base)
                      ie




                                       c                                     c
                       ic                                            ic                   h fe rC
                       acib                                         acib       Av  
                                                   ac+1)r'e                              hie
    b                                          b
             ib                                     ib
                      r'e                                                                    Zin rC 
                      ie                                            ie           Ai  h fe         
                                                                                             hie RL 
                  e                                             e
                                                                                                         53
  Determining h-Parameter Values

Use geometric means if given max. and min.
values.

                hie  hie(min)  hie(max)

                h fe  h fe(min)  h fe(max)



See examples 9.18 and 9.19.

                                               54
            Summary
• AC concepts
• Roles of capacitors in amplifiers
• Common-emitter ac equivalent
  circuit
• Amplifier gain
• Gain and impedance calculations
• Swamped amplifiers
• h-parameters

                                      55

						
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