Page 33 - Physics_Form_2
P. 33

Static electricity


                                                      their  total  capacitance,  C, can  be obtained
                ,
           If  V V 2 , and V are potential differences   using equation (3) as follows:
               1
                          3
           are developed between the various plates,
           then  the  total  potential  difference,  V,       1    1    1
           across AD is:                                      C  =  C 1  +  C 2

          FOR ONLINE READING ONLY
                  V =  V +  1  V +  2  V                  (1)      CC
                               3
                                                              C =    1  2
                                                                    1
           When capacitors are in series, there is an             C + C 2
           equal distribution of charge on the plates.
           Charge Q on  C  is transferred to  C  and       Example 1.3
                                              2
                          1
           C  by induction. Then,                      Three capacitors, labeled A, B, and C,
             3
                    Q        Q             Q           have capacitances of 10 μF, 20 μF, and
               V =  C  , V =  C  , and V =  C          30 μF, respectively, and are connected
                         2
                 1
                                       3
                              2
                     1
                                            3
                                                       in  series.  Find the  value  of a  single
           Substituting   ,V V 2 , and V  into equation   capacitor that could replace them.
                          1
                                    3
           (1), you get;
                                                       Solution
                    V =  Q  +    Q  +    Q            (2)  Use the formula for capacitors in series.
                   C 1  C 2  C 3                              1    1    1    1
                       1   1    1                           C  =  C  +  C  +  C
               V   Q              but, V =  Q                  1    2    3
                       C 1  C 2  C 3        C               1      1       1       1
                                                                               
                                                              C   10 μF   20 μF 30 μF
           Where C is the combined or equivalent
           capacitance.                                    632       11
                                                                   
                  Q       1   1    1                      60 μF     60 μF
           Then,      Q             ,
                  C       C 1  C 2  C 3                         60 μF
                                                              C           5.45 μF

           Simplifies to:                                           11
                                                       Therefore,  the value  of an equivalent
                 1     1   1    1                    single capacitor is 5.45 μF.
                       C          C 1       C 2    C 3                   (3)

                                                      Capacitors in parallel
           Therefore, Equation (3) is used to calculate   In a parallel arrangement, all capacitors
           the total capacitance of the three capacitors   have the same potential difference across
           connected in series.                       them, as shown in Figure 1.37. However,

           Thus,  if  two  capacitors  are  in  series,  then   the charges for all capacitors are different.


                                                                                         27




     Physics Form 2 Final.indd   27                                                         25/10/2025   10:25
   28   29   30   31   32   33   34   35   36   37   38