Page 12 - Electrostatics-11
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                                                                   1  1
                                               = −           ∫            
                                                     4     0      2     2


                                                                   1
                                               = −           ∫      −2     
                                                     4     0      2


                                                                  −2+1      1
                                             = −             [         ]
                                                    4     0   −2 + 1        2


                                                                1     1
                                               = −             [   −     ]
                                                      4     0     1      2


                                                                  −    1
                                                                 2
                                               = −             [         ]
                                                      4     0       .    2
                                                                  1
        By  definition,  this  work  done  is  electric  potential  difference  (V).
                                                                       −    1
                                                                     2
                                           ∴         = −           [         ]
                                                          4     0       .    2
                                                                      1

        This is the required expression for electric potential difference between points A
        and B.





        Electric potential  at a point due to number of charges:

               Electric potential at a point due to the number of charges is the sum of electric

        potentials due to individual charges.




                                      P

                                                       rn
                             r1

                                                  r3                 Qn
                                         r2

                  Q1
                                                             Q3

                                       Q2


                              V = V1 + V2+ V3+ ... ... ... + Vn





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