Page 99 - Mechanical Engineers Reference Book
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2/40  Electrical and electronics principles
     Kirchhoff's  first  law,  it  is  apparent  that  il  = -i2. Thus  VI/
     R1  = -V,/Rz,  and the gain can be written as
                                            (2.108)

       Provided the open-circuit gain of the amplifier is very high,
     the overall gain with this negative feedback system is given by
     the ratio of the two external resistors and is independent of the
      open-circuit gain.


     2.3.14.2  Unity gain amplifier
      Figure 2.80 depicts a unity gain amplifier in which no external
      resistors are wired into the circuit. The unity gain amplifier is
      also known as a voltage follower or as a buffer amplifier. This
      type  of  amplifier  circuit  is  often  used  in  instrumentation
      systems where the internal resistance  of  a voltage-generating
      transducer and that of the voltage-recording instrument are so
      poorly  matched  that the transducer  voltage  is seriously atte-
      nuated.  This  situation  arises  when  the  transducer  internal   Figure 2.81  Non-inverting amplifier
      resistance  is  large  in  comparison  to  that  of  the  recording
      instrument.  Since  the  buffer  amplifier  has  a  large  input
      impedance  and a low output impedance  it can be interfaced   Hence
      between  the  transducer  and  the  recording  instrument  to   vo   R2  + Rl
      provide  optimum  impedance  matching.  This  gives  a  low   -
      source  impedance  and  high  destination  impedance  between   Vi   RI
      both  the  transducer  and  amplifier  and  also  between  the   Since E is a virtual earth, then  Vi = VI and
      amplifier and the instrument.
                                                    V,  R2  + Ri
       Summing the voltages  round  the  amplifier  in  Figure  2.80   --___              (2.110)
                                                       -
      gives                                          v1    R1
      v, + v, = vn                                  If, in addition, R2 9 R1,
      Since the internal impedance of the amplifier is very large then   - -5
                                                     Vn
                                                       -
      V, is effectively zero and the gain is                                              (2.111)
                                                     v1   R1
      vo/vl = 1                             (2.109)
                                                    2.3.14.4  Summing amplifier
                                                    The summing amplifier is shown in Figure 2.82. As point E is a
      2.3.14.3  Non-inverting amplifier             virtual earth, then
      Figure 2.81 shows the operational amplifier connected up for a   -id  = il + iz + i3
      non-inverting  output.  Assuming  that  the  currents  through
      resistors R1 and R2 are equal and that point E is a virtual earth,   Therefore
      vi   v, - vi                                   VO
        -
      Rl    R2                                       R4





















      Figure 2.80  Unity gain amplifier              Figure 2.82  Summing amplifier
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