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                        JWST499-Cetinkunt
                                                       ELECTRONIC COMPONENTS FOR MECHATRONIC SYSTEMS  307
                                          –                                   –
                             Solar
                              cell        +                                   +








                             FIGURE 5.39: Example op-amp circuits: (a) current-to-voltage converter op-amp circuit used
                             to provide output voltage that is proportional to the current generated by the solar cell, (b)
                             voltage-to-current converter op-amp circuit where the intensity of LED light is proportional to
                             the current, which is proportional to the input voltage pickup by the adjustable resistor R 3 .


                             Example     Show that the following Figures 5.40a and b represent a low pass and a high
                             pass filter, like those shown in Figure 5.36, except that the sign of the input–output gain is
                             negative.

                                                    V out (s)  =−  1  ;  low pass              (5.301)
                                                    V (s)     RCs + 1
                                                     in
                                                    V out (s)  RCs
                                                          =−        ;  high pass               (5.302)
                                                    V (s)     RCs + 1
                                                     in
                             where R = R = R is assumed.
                                         2
                                    1
                                  The transfer function in the frequency domain between input and output voltages
                             can be derived by following the op-amp idealized assumptions and Kirchoff’s current and
                             voltage laws. Consider the low pass filter. The voltage at the positive terminal is grounded,
                                                                                         +
                                                                                              −
                             hence the voltage potential at the negative terminal is also grounded since v = v ,
                                                               +
                                                              v = 0                            (5.303)
                                                               −
                                                              v = 0                            (5.304)



                                                   C                                 R 2

                                                 R  2
                                   R 1                                C   R 1



                             V i                                   V i
                                                           V o                                   V o






                                           (a)                                    (b)
                             FIGURE 5.40: (a) Low pass, inverting, active filter, (b) high pass, inverting, active filter.
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