Page 10 - 6413
P. 10


                                                                 F
                                                            E                                         (2.1)
                                                                  q
                         The intensity of the electric field at the given point of space is a
                  physical quantity that equals the ratio of the force F, with which the

                  electric field affects the unit, at positive point, tests the charge located
                  at the given point to the value of test charge q.
                         The electric field is a vector field and can reveal you what force

                  charge experiences at a particular position in space. While researching
                  the electric field around a charge, it is important for the test charge to
                  be comparatively negligible on the field-producing charge. This will

                  ensure  that  the  introduction  of  the  test  charge  does  not  change  the
                  field-producing charge arrangement. Since the direction of the force
                  on the charge depends on whether the charge is positive or negative,
                  this  must  be  specified  in  a  field  representation.  By  convention,  a

                  positive test charge q is used for measuring the field. The SI unit for
                                                                               N
                  the electric field is the newton per coulomb   or volt per meter
                                                                                  C
                   V
                   .
                      m















                                                            Figure 2.1

                         The magnitude of the electric field (E) in the space point A at a
                  distance  of  r  (Fig.  2.1)  from  the  point  charge  q   is  then  easily
                                                                                       0
                  computed according to Coulomb's force law

                                                       q  q
                                                        0
                                             F     4      r    2   q
                                       E              0               0                             (2.2)
                                             q          q          4      r    2
                                                                        0






                                                                  9
   5   6   7   8   9   10   11   12   13   14   15