Potential Energy In External Field Assignment Help

Electrostatics - Potential Energy In External Field

Potential Energy in External Field

~ - Represents Vector

Potential energy of a single charge in an external field

We have already obtained an expression for potential energy of a system of charges. In this case, the source of the electric field, i.e. charges and their locations – was specified.

We have now to determine potential energy of a charge (or charges) in an external field ~E - which is not produced by the given charges whose potential energy we have to calculate. The sources which produce external field ~E are often unknown and they are of no interest to us.

The external electric field ~E  and the corresponding external potential V may change from point to point. IfV (~r) is extended potential at any point P of position vector ~r, then by definition, work done in bringing a unit positive charge from infinity to the point P is equal to V.

Therefore, work done is bringing a charge q from infinity to the point P in the external field = q . V (~r).

This work is stored in the charged particle in the form of its potential energy.

Potential energy of a single charge q at ~r in an external field = q . V (~r).
    
Potential energy of a system of two charges in an external field

Suppose q1, q2 are two mid point charges at position vectors  ~r1 and ~r2 respectively, in a uniform external electric field of intensity ~E To calculate the potential energy of the system of these two charges in the external field, we find that

Work done in bringing charge q1 from infinity to position ~r1 is W1 = q1 . V (~r1 where V (~r1 ) is potential at ~r1 due to external field.


Again, work done in bringing charge q2 from infinity to position ~r2   against the external field is W2 = q2 . V (~r2) where V (~r2) is potential at ~r2  due to external field.


While bringing q2 from infinity to position  ~r2  , work has also to be done against the field due to q1. This is  

W3 = q1q2/4∏?0   ~r12 

Where  ~r12  is the distance between q1 and q2.

By the superposition principle, we add up the work done and find P.E. of the system = total work done in assembling the charge configuration

U = q1 . V (~r1) + q2 . V  (~r2  ) + q1q2/4∏?0 ~r12 

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