Consider the following distribution of charges: two +1
charges
are placed at opposite corners, A and C, of a 1 cm square. A negative
charge Q of -4
is put in corner B.
(b) The electric field at D has 3 contributions. Those due to charges
A and C are both repulsive, and give a vector sum pointing in
direction d. The contribution due to charge B is attractive, and points
in direction b. The net electric field is the vector sum of both
contributions, with its direction depending on the magnitudes of the
attraction along b and repulsion along d. The attractive field along b
due to charge B has magnitude
. The repulsive field is the sum of vectors due to charges A
and C, each with magnitude
. Thus there is no way that the two repulsive forces, pointing
in perpendicular directions, can sum to a contribution along d which
is large enough to overcome the greater attractive field along b. Thus
the net electric field points along b.
(c) Field lines exit positive charges, and enter negative ones. The
number of field lines entering or exiting a charge must be
proportional to its charge; thus if 2 field lines exit each
charge, then 8 field lines must enter the
charge. (c)
satisfies both these criteria.
BY. Positive work done by the electric force reduces the electric potential energy (it transfers potential energy to kinetic energy). Here the electric potential decreases, so the electric potential energy of our positive test charge decreases, as we move from spatial infinity to D. Thus positive work is done by the electric force. The opposite, negative work is done against it.
The work done by the electric force gives the decrease in the test charge's electric potential energy:
The electric potential at point D is the sum of (scalar) contributions from charges A, B, and C. Charges A and C contribute
Thus, to obtain zero potential at D, charge B must contribute the opposite potential
Solving for Q gives