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NIOS Final Exam Focus

Lesson 16: Electric Potential and Capacitors

This chapter usually gives direct theory questions, derivations, and capacitor numericals. Revise definitions, formulas, and comparisons carefully.

1. Electric Potential

  • Electric potential at a point is the work done in bringing a unit positive charge from infinity to that point.
  • Potential is a scalar quantity.
  • SI unit of potential is volt (V).
  • Potential difference is work done per unit charge between two points.
  • Work done in electrostatic field is path independent.

V = W/q and VB - VA = WAB/q

2. Potential due to Point Charge

  • Potential due to a point charge varies as 1/r.
  • For positive charge, potential is positive.
  • For negative charge, potential is negative.
  • If many charges are present, total potential is algebraic sum, not vector sum.

V = (1/4πε0) (q/r)

3. Potential due to Electric Dipole

  • Potential due to dipole depends on distance and angle.
  • It varies as 1/r2.
  • On axial line, potential is maximum in magnitude.
  • On equatorial line, potential is zero.

V = (1/4πε0) (p cos θ/r2)

4. Equipotential Surfaces

  • All points on an equipotential surface have same potential.
  • No work is done in moving a charge on an equipotential surface.
  • Electric field is always perpendicular to the equipotential surface.
  • Two equipotential surfaces never intersect.

5. Potential Energy

  • Potential energy of a system is the work done in assembling charges from infinity.
  • For like charges, potential energy is positive.
  • For unlike charges, potential energy is negative.
  • For a dipole in uniform electric field, potential energy depends on angle.

U = (1/4πε0) (q1q2/r), U = -pE cos θ

6. Relation Between Electric Field and Potential

  • Electric field is equal to negative potential gradient.
  • Negative sign shows potential decreases in the direction of electric field.
  • If potential is constant in a region, electric field is zero there.

E = -dV/dr and for uniform field E = (VA - VB)/d

7. Conductors in Electrostatic Equilibrium

  • Electric field inside a conductor is zero.
  • Any excess charge resides on the outer surface.
  • Electric field at the surface is perpendicular to the conductor.
  • Cavity inside a conductor is shielded from external electric field.
  • This is the basis of electrostatic shielding.

8. Capacitance

  • A capacitor stores charge and electrical energy.
  • Capacitance is the ratio of charge to potential difference.
  • SI unit is farad (F).
  • Capacitance depends on size, shape, and medium, not on material alone.

C = Q/V

9. Important Capacitor Formulas

  • Capacitance of isolated spherical conductor is directly proportional to radius.
  • For parallel plate capacitor, capacitance increases with plate area and decreases with separation.
  • If dielectric is inserted, capacitance increases by factor K.

Sphere: C = 4πε0r
Parallel plate: C0 = ε0A/d
With dielectric: C = Kε0A/d = KC0

10. Dielectric Constant

  • Relative permittivity or dielectric constant is denoted by K or εr.
  • It compares a medium with vacuum.
  • It can be expressed using force or capacitance ratio.

K = ε/ε0 = Fvac/Fmedium = C/C0

11. Grouping of Capacitors

  • In parallel, potential difference is same across each capacitor.
  • In parallel, equivalent capacitance is greater than each individual capacitance.
  • In series, charge is same on each capacitor.
  • In series, equivalent capacitance is less than the smallest capacitor.

Parallel: Cp = C1 + C2 + C3 + ...
Series: 1/Cs = 1/C1 + 1/C2 + 1/C3 + ...

12. Energy Stored in a Capacitor

  • Charging a capacitor requires work.
  • This work is stored as electrostatic potential energy.
  • Energy increases with capacitance and with square of potential difference.

U = (1/2)CV2 = (1/2)QV = Q2/(2C)

13. Dielectric Polarization

  • Non-polar dielectrics have no permanent dipole moment in normal state.
  • Polar dielectrics already have permanent dipole moment.
  • In external electric field, dielectric gets polarized.
  • Polarization creates an opposing field inside dielectric.
  • Effective field decreases, so capacitance increases.

Eeffective = E - Ep

14. NIOS Exam Traps

  • Potential is scalar, electric field is vector.
  • Potential can be zero while electric field is not zero, for example on equatorial line of a dipole.
  • If electric field is zero in a region, potential may be zero or constant.
  • For capacitors in series, same charge; for parallel, same potential difference.
  • Insertion of dielectric usually increases capacitance.

15. High-Value Questions to Prepare

  • Derivation of potential due to a point charge.
  • Derivation of capacitance of parallel plate capacitor.
  • Series and parallel combination of capacitors.
  • Energy stored in a capacitor.
  • Electrostatic shielding and behavior of conductors in electric field.
  • Effect of dielectric on capacitance.

Best revision method: learn one formula with meaning, unit, and one line about where it is used.