# Energy Density in Electrostatic Fields

To determine the Energy present in an assembly of charges (or) group of charges one must first determine the amount of work necessary to assemble them.

It is seen that , when a unit positive charge is moved from infinity to a point in a field, the work is done by the external source and energy is expended.

If the external source is removed then the unit positive charge will be subjected to a force exerted by the field and will be moved in the direction of force.

Thus to hold the charge at a point in an electrostatic field, an external source has to do work , this energy gets stored in the form of Potential Energy when the test charge is hold at a point in a field.

when external source is removed , the Potential Energy gets converted to a Kinetic Energy.

In order to derive the expression for energy stored in electrostatics (i.e, the expression of such a Potential Energy)

Consider an empty space where there is no electric field at all, the Charge is moved from infinity to a point in the space ,let us say the point as , this requires no work to be done to place a charge from infinity to a point in empty space. i.e, work done = 0 for placing a charge from infinity to a point in empty space.

now another charge has to be placed from infinity to another point . Now there has to do some work to place at because there is an electric field , which is produced by the charge and is required to move against the field of .

Hence the work required to be done is

i.e, .

Work done to position at = .

Now the charge to be moved from infinity to , there are electric fields due to and , Hence total work done is due to potential at due to charge at and Potential at due to charge at .

Work done to position at = . Similarly , to place a  charge at in a field created by (n-1) charges is ,work done to position at

Total Work done

The total work done is nothing but the Potential energy in the system of charges hence denoted as ,

if charges are placed in reverse order (i.e, first and then and then    and finally is placed)

work done to place

work done to place

work done to place

Total work done

EQN (I)+EQN(II) gives

let , and are the resultant Potentials due to all the charges except that charge.

i.e, is the resultant potential due to all the charges except .

Joules.

The above expression represents the Potential Energy stored in the system of n point charges.

simillarly,

Joules

Joules

Joules  for different types of charge distributions.     (No Ratings Yet) Loading... ## Author: vikramarka

Completed M.Tech in Digital Electronics and Communication Systems and currently working as a faculty.

Posted on Categories Electro Magnetic Theory