Page 273 - Mechatronics with Experiments
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                        JWST499-Cetinkunt
            JWST499-c05
                                                       ELECTRONIC COMPONENTS FOR MECHATRONIC SYSTEMS  259
                             and the output voltage is affected by the output impedance,
                                                               R L
                                                       V out  =      K amp  V in                (5.79)
                                                             R + R out
                                                              L
                             Notice that the ideally, when R → ∞ and R  → 0, V = v and V  = K  v , where the
                                                     in         out     in   s    out   amp s
                             input and output loading effects are zero. In reality, the finite input and output impedance
                             introduces so-called loading errors to the signal amplification. This is minimized when
                             the input impedance is very large relative to the source impedance, and output impedance
                             is very small relative to the load impedance. The net gain of the amplifier in a real
                             amplifier is
                                                     (         )(        )
                                                          R L       R in
                                                 v =                        K amp s             (5.80)
                                                                                v
                                                  o
                                                       R + R out  R + R s
                                                                    in
                                                        L
                             where the portion of the amplifier gain
                                                             R L    R in
                                                          R + R   R + R                         (5.81)
                                                           L    out  in  s
                             is due to the input and output loading effects. In order to minimize the effect of input
                             loading errors,

                                                              R ≫ R s                           (5.82)
                                                               in
                             Similarly, in order to minimize the output loading errors,
                                                             R out  ≪ R L                       (5.83)

                                  Furthermore, more accurate analysis of the amplifier would take the frequency depen-
                             dance of the input and output impedance into account (Z (jw) instead of R , Z out (jw) instead
                                                                                       in
                                                                         in
                             of R out ).
                             Example     Let us consider a sensor, a signal amplifier, and a measurement device, all
                             connected in series as shown in Figure 5.8. The sensor provides a voltage proportional to the
                             measured physical variable. Let us call that voltage v (t) = 10 V at steady-state condition.
                                                                        s
                             For simplicity let us assume that the gain of the amplifier is unity, K amp  = 1.0. Determine
                             the voltage measured at the measuring device (i.e., digital voltmeter or oscilloscope) for
                             the following two conditions,

                                1. R = 100 Ω, R = 100 Ω, R = 100 Ω, R out  = 100 Ω
                                              L
                                                         in
                                   s
                                2. R = 100 Ω, R = 100 Ω, R = 1 000 000 Ω, R out  = 1 Ω
                                   s
                                                         in
                                              L
                                  For the first case, the measured voltage is
                                                      (        )(        )
                                                          R L       R in
                                                                                v
                                                 v out  =                   K amp s             (5.84)
                                                        R + R o   R + R s
                                                         L
                                                                    in
                                                      (   100   )(    100   )
                                                    =                         1 v s             (5.85)
                                                        100 + 100  100 + 100
                                                    = 0.25 ⋅ v                                  (5.86)
                                                            s
                                                    = 2.5 V                                     (5.87)
                             which shows an error of 75% of the correct value of the voltage.
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