Electric field due to the system of point charges:
Suppose a number of point charges are distributed in space. To find the electric field at some point P due to this collection of point charges, superposition principle is used. The electric field at an arbitrary point due to a collection of point charges is simply equal to the vector sum of the electric fields created by the individual point charges. This is called superposition of electric fields.
Consider a collection of point charges q1, q2, q3,…., qn located at various points in space. The ‘ total electric field at some point P due to all these n charges is given by
Here r1p, r2p, r3p,…., rnp, are the distance of the charges q1, q2, q3,…., qn from the point respectively. Also \(\hat r\)1p + \(\hat r\)2p + \(\hat r\)3p ,…., \(\hat r\)np are the corresponding unit vectors directed from q1, q2, q3, ....., qn to point P.
Equation (2) can be re-written as,
For example in figure, the resultant electric field due to three point charges q1, q2, q3 at point P is shown. Note that the relative lengths of the electric field vectors for the charges depend on relative distantes of the charges to the point P.