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Electric Field and Potential

This section was requested by Ajay, Mitali, and Sravan

1 What is electricity, static electricity? Charges are of two types....

etc... etc... etc....

You all know this basic stuff by now..

No point wasting time on such basic ideas

Let's move on to other important things

2 Charge is conserved (remember conservation of momentum!) Charge cannot be created or destroyed
3 Charge is relativistically invariant Charge does not change with velocity

(remember how mass changes with velocity)

4 Charge has quantum nature, with the smallest unit being e e = 1.6x 10-19 C (charge on an electron)
5 Coulomb's Law

Force is directly proportional to the product of charges, inversely proportional to square of distance between them. Notice the similarity with the formula for gravitational force.

6 Electric Field A region in which a charged particle experiences
a force
7 Electric Field Strength Force experienced by a unit positive charge at a point
8 Properties of lines of force:

They diverge (start) from a positive charge and converge (end) at a negative charge

They are closer together in regions where the field is stronger and further apart where the field is weak.

They begin and end perpendicularly to the charged surface

They never cross.

The lines of force are always directed from higher to lower potential

the field is continuous, while they are drawn as lines at discrete
intervals

9 Charge is a scalar quantity.

Force is a vector quantity

10 The presence of a charge creates an electric field in space, the strength of which is a vector quantity.
The force between two positive charges is directed along the line
joining these charges.
11 If the sign of the charges is included in calculations of the force between two charges using Coulomb's Law, then the forces which have a negative sign are attractive and those which have a positive sign are repulsive.
Opposite charges attract, same charges repel
12 Strength of Field due to an electric charge

Strength of field due to a group of point charges

E = F/q0

E = E1+E2+E3+..... (Remember this is a vector addition.
Do not add them directly. Do not forget the cos_theta !)

13 Electric Flux


Flux is a measure of the number of field lines passing through an
area.

Φ E = E · A = E A cos(θ)

where θ is the angle between the electric field and the area vector.

14 Gauss Theorem The net electric flux through a closed surface = 1/ε0 times net charge enclosed within
15 Electric Potential (at a point) Work done to move a unit positive charge from infinity to that
point
16 Electric potential at a point V(r) = q / 4 π&epsilon0 r
17 Electric Dipole

Two equal and opposite charges separated by by a distance 2l

Dipole Moment p = q x (2l) Note that entities in bold are vectors. The direction is from negative to positive charge.
18 The torque on a adipole in a uniform electric field τ = pE sin&theta
19 Work done in rotating a dipole through angle &theta from equilibrium W = pE(1 - cos &theta)
20 Potential energy of dipole U = - pE cos &theta
21 Electric potential energy between two point charges (1 and 2) U12 = q1q2 / 4 π&epsilon0 r12
22 Electric potential energy for a system of charges (lets say 3 charges 1,2, and 3) U = U12 + U13 + U23
23 Electric field due to a dipole The total electric field due to the dipole is the vector sum of the fields due to each charge at any location.

(Tip: Do not forget cos &theta )

24 Some interesting cases that you must consider for exam Electric field and potential due to a charged spherical conductor/non-conductor: inside/ on surface/ outside

Motion of a charged particle in an electric field (Remember Force = mass X acceleration = qxE)

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The topics covered in this section are written in a language to cover more important concepts in minimum time.

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