# Physics 12th Electric Potential

- On 05/03/2013
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## ELECTRIC POTENTIAL

**1. Introduction**

- We already have an introduction of work and energy while studying mechanics.
- We know that central forces are conservative in nature i.e., work done on any particle moving under the influence of consrevative forces does not depend on path taken by the particle but depends on initial and final positions of the particle.
- Electrostatic force given by Coulumb's law is also a central force like gravitational force and is conservative in nature.
- For conservative forces, work done on particle undergoing displacement can be expressed in terms of potential energy function.
- In this chapter we will apply work and energy considerations to the electric field and would develop the concept of electric potential energy and electric potential.

**2. Electric potential energy**

- Conside a system of two point charges in which positive test charge q' moves in the field produced by stationary point charge q shown below in the figure.
- Charge q is fixed at point P and is displaced from point R to S along a radial line PRS shown in the figure.
- Let r
_{1}be the distance between points P and R and r_{2}be the distance between P and S. - Magnitude of force on positive test charge as given by Coulumb's law is

- If q' moves towards S through a small displacement d
**r**then work done by this force in making the small displacement d**r**is

dW=**F**·d**r**

- Total work done by this force as test charge moves from point R to S i.e., from r
_{1}to r_{2}is,

or

- Thus for this particular path work done on test charge q' depends on end points not on the path taken.
- Work done W in moving the test charge q' from point R to S is equal to the change in potential energy in moving the test charge q' from point R to S. Thus,

W=U(r_{1})-U(r_{2}) (4)

where

is the potential energy of test charge q' when it is at point R and

is the potential energy of test charge q' when it is at point S. - Thus potential energy of test charge q' at any distance r from charge q is given by

Equation 5 gives the electric potential energy of a pair of charges which depends on the separation between the charges not on the location of charged particles. - If we bring the test charge q' from a very large distance such that r
_{2}=∞ to some distance r_{1}=r then we must do work against electric forces which is equal to increase in potential energy as given by equation 5. - Thus potential energy of a test charge at any point in the electric field is the work done against the electric forces to bring the charge from infinity to point under consideration.

**3. Electric Potential**

- We now move towards the electric potential which is potential energy per unit charge.
- Thus electrostatic potential at any point of an electric field is defined as potential energy per unit charge at that point.
- Electric potential is represented by letter V.

V=U/q' or U=q'V (6) - Electric potential is a scalar quantity since both charge and potential energy are scalar quantities.
- S.I. unit of electric potential is Volt which is equal to Joule per Coulumb. Thus,

1 Volt = 1 JC^{-1} - In equation 4 if we divide both sides by q' we have

where V(r_{1}) is the potential energy per unit charge at point R and V2) is potential energy per unit charge at point S and are known as potential at points R and S respectively. - Again consider figure 1. If point S in figure 1 would be at infinity then from equation 7

Since potential energy at infinity is zero therefore V(∞)=0. Therefore

hence electric potential at a point in an electric field is the ratio of work done in bringing test charge from infinity to that point to the magnitude of test charge. - Dimensions of electric potential are [ML
^{2}T^{-3}A^{-1}] and can be calculated easily using the concepts of dimension analysis.

**4. Electric potential due to a point charge**

- Consider a positive test charge +q is placed at point O shown below in the figure.
- We have to find the electric potential at point P at a distance r from point O.
- If we move a positive test charge q' from infinity to point P then change in electric potential energy would be

- Electric potential at point P is

- Potential V at any point due to arbitrary collection of point charges is given by

- here we see that like electric field potential at any point independent of test charge used to define it.
- For continous charge distributions summation in above expressin will be replaced by the integration

where dq is the differential element of charge distribution and r is its distance from the point at which V is to be calculated.

**5. Relation between electric fiels and electric potential**

- Consider the electric field E due to a point charge +q at point O in a radially outward direction shown below in the figure.
- Suppose R and S are two points at a distance r and r+dr from point O where dr is vanishingly small distance and V is electric potential at point R.
- Now force on any test charge q' at point R in terms of electric field is
**F**=q'**E** - Work done by the force in displacing test charge from R to S in field of charge q is

dW =**F**·d**r**= q'**E**·d**r**

and, change in potential energy is

dU = -dW = -q'**E**·d**r**

Change in electric potential would be

dV = dU/q

or dV = -**E**·d**r**(11) - From equation 11 electric field is

E=-(dV/dr) (12)

the quantity dV/dr is the rate of change of potential with the distance and is known as potential gradient. Negative sign in equation 12 indicates the decrease in electric potential in the direction of electric field. - For cartesian coordinate system
E=E _{x}i+E _{y}j+E _{z}k

and,

dr=dx i+dy j+dz k

from equation 11

dV=-E⋅d r

or, dV=-(E_{x}dx+E_{y}dy+E_{z}dz) (13) - Thus components of
E are related to corresponding derivatives of V in the following manner

E_{x}=dV/dx (14a)

E_{y}=dV/dy (14b)

E_{z}=dV/dz (14c)

In equation (14a) we see that V is differentiated with respect to coordinate x keeping other coordinates constant. Same is the case with equations (14b) and (14c) in case of y and z coordinates respectively.

**6. Equipotential surfaces**

- Surface over which the electric potential is same everywhere is called an equipotential surface.
- Equipotential surfaces are graphical way to represent potential distribution in an electric field.
- We can draw equipotential surfaces through a space having electric field.
- For a positive charge , electric field would be in radially outward direction and the equipotential surfaces would be concentric spheres with centers at the charge as shown below in the figure.
- Since electric potential remains same everywhere on an equipotential surface from this it follows that PE of a charged body is same at all points on this surface.This shows that work done in moving a charged body between two points on an equipotential surface would be zero.
- At every point on equipotential surface electric field lines are perpandicular to the surface. This is because potential gradient along any direction parallel to the surface is zero i.e.,

E=-dV/dr=0

so component electric parallel to equipotential surface is zero.

**7. Potential due to an electric dipole**

- We already know that electric dipole is an arrangement which consists of two equal and opposite charges +q and -q separated by a small distance 2a.
- Electric dipole moment is represented by a vector
**p**of magnitude 2qa and this vector points in direction from -q to +q. - To find electric potential due to a dipole consider charge -q is placed at point P and charge +q is placed at point Q as shown below in the figure.
- Since electric potential obeys superposition principle so potential due to electric dipole as a whole would be sum of potential due to both the charges +q and -q. Thus

where r_{1}and r_{2}respectively are distance of charge +q and -q from point R. - Now draw line PC perpandicular to RO and line QD perpandicular to RO as shown in figure. From triangle POC

cosθ=OC/OP = OC/a

therefore OC=acosθ similarly OD=acosθ

Now ,

r_{1}= QR≅RD = OR-OD = r-acosθ

r_{2}= PR≅RC = OR+OC = r+acosθ

since magnitude of dipole is

|**p**| = 2qa

- If we consider the case where r>>a then

again since pcosθ=**p**·**rˆ**where,**rˆ**is the unit vector along the vector OR then electric potential of dipole is

for r>>a - From above equation we can see that potential due to electric dipole is inversly proportional to r
^{2}not ad 1/r which is the case for potential due to single charge. - Potential due to electric dipole does not only depends on r but also depends on angle between position vector
**r**and dipole moment**p**.

**8. Work done in rotating an electric dipole in an electric field**

- Consider a dipole placed in a uniform electric field and it is in equilibrium position. If we rotate this dipole from its equllibrium position , work has to be done.
- Suppose electric dipole of moment
**p**is rotated in uniform electric field**E**through an angle θ from its equilibrium position. Due to this rotation couple acting on dipole changes. - If at any instant dipole makes an angle φ with uniform electric field then torque acting on dipole is

Γ=pEsinφ (19)

again work done in rotating this dipole through an infitesimaly small angle dφ is

dW=torque x angular displacement

=pEsinφdφ - Total work done in rotating the dipole through an angle θfrom its equilibrium position is

This is the required formula for work done in rotating an electric dipole placed in uniform electric field through an angle θ from its equilibrium position.

**9.Potential energy of dipole placed in uniform electric field**

- Again consider equation 20 which gives the work done in rotating electric dipole through an infinetesimly small angle dφ is

dW=pEsinφdφ

which is equal to the change in potential energy of the system

dW=dU=pEsinφdφ (22) - If angle dφ is changed from 90
^{0}to θ then in potential energy would be

- We have choosen the value of φgoing from π/2 to θ because at π/2 we can take potential energy to be zero (axis of dipole is perpandicular to the field). Thus U(90
^{0})=0 and above equation becomes