Electrostatic Potential and Capacitance
Class 12 Physics • CBSE 2025-26 Syllabus
Click any section header to expand and explore the content
Key Concepts and Tricks
+Essential concepts you need to master for electrostatic potential and capacitance. These form the foundation for understanding energy storage and electrical systems.
Electrostatic Potential
Work done per unit positive test charge in bringing it from infinity to that point. It's a scalar quantity measured in volts (V).
Potential vs Potential Energy
Potential V = U/q. Potential is energy per unit charge, while potential energy depends on the amount of charge present.
Potential due to Point Charge
V = kQ/r. Positive charges create positive potential, negative charges create negative potential. Potential is scalar - no direction.
Potential due to Electric Dipole
On axis: V = 2kp cos θ/r². On equatorial line: V = 0. Falls off as 1/r² unlike single charge (1/r).
Equipotential Surfaces
Surfaces where potential is constant. Always perpendicular to electric field lines. No work needed to move charge on these surfaces.
Relation between E and V
Electric field E = -dV/dr. Field points in direction of steepest decrease of potential. Field and potential are related but different.
Conductors in Electrostatics
Electric field inside = 0. Potential is constant throughout. All charges reside on surface. Field at surface is perpendicular.
Dielectrics and Polarization
Insulating materials that reduce electric field when placed between capacitor plates. Characterized by dielectric constant K.
Capacitance Concept
C = Q/V. Ability of a system to store electric charge. Depends on geometry and dielectric material. Unit: Farad (F).
Energy Storage in Capacitors
U = ½CV² = ½QV = ½Q²/C. Energy stored in electric field between plates. Important for electronic circuits and power systems.
Important Formulas
+All essential formulas with clear explanations. Make sure you understand when and how to apply each one.
| Formula Name | Mathematical Expression | Simple Explanation |
|---|---|---|
| Potential due to Point Charge | $V = \frac{kQ}{r}$ | Potential at distance r from point charge Q |
| Potential due to Dipole (Axial) | $V = \frac{2kp \cos \theta}{r^2}$ | Potential on axis of dipole at distance r >> a |
| Potential due to System of Charges | $V = \frac{k}{4\pi\varepsilon_0} \sum \frac{q_i}{r_i}$ | Algebraic sum of potentials due to individual charges |
| Electric Field and Potential Relation | $E = -\frac{dV}{dr}$ | Electric field is negative gradient of potential |
| Potential Energy of Two Charges | $U = \frac{kq_1q_2}{r_{12}}$ | Work done to bring charges from infinity to separation r₁₂ |
| Dipole Energy in External Field | $U = -\vec{p} \cdot \vec{E}$ | Energy of dipole in uniform external electric field |
| Capacitance Definition | $C = \frac{Q}{V}$ | Ratio of charge to potential difference |
| Parallel Plate Capacitor | $C = \frac{\varepsilon_0 A}{d}$ | Capacitance depends on area A and separation d |
| Effect of Dielectric | $C = KC_0$ | Dielectric increases capacitance by factor K |
| Capacitors in Series | $\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3}$ | Reciprocals of capacitances add in series |
| Capacitors in Parallel | $C = C_1 + C_2 + C_3$ | Capacitances add directly in parallel |
| Energy Stored in Capacitor | $U = \frac{1}{2}CV^2 = \frac{1}{2}QV = \frac{Q^2}{2C}$ | Energy stored in electric field of capacitor |
Step-by-Step Problem Solving
+Follow these systematic steps to solve any electrostatic potential and capacitance problem with confidence.
Identify Problem Type
Determine if it's potential calculation, capacitance problem, or energy storage question
Draw Clear Diagram
Show all charges, distances, capacitors, and electrical connections clearly
Choose Reference Point
Usually take potential zero at infinity for isolated charges
Apply Superposition
For multiple charges, add potentials algebraically (scalar addition)
Identify Circuit Configuration
For capacitors, determine series/parallel combinations and simplify step by step
Check Units and Signs
Verify units are consistent (V, F, J) and signs follow physics conventions
Validate Answer
Check using energy conservation, limiting cases, or physical reasoning
Common Mistakes to Avoid
+Learn from these common pitfalls that students often encounter. Knowing what to avoid is as important as knowing what to do.
| Common Mistake | How to Avoid It |
|---|---|
| Confusing electric potential and potential energy | Remember V = U/q. Potential is per unit charge, energy depends on actual charge |
| Wrong signs in potential calculations | Positive charges always give positive potential, negative charges give negative potential |
| Mixing up series and parallel capacitor formulas | Series: reciprocals add (like resistors in parallel). Parallel: direct addition |
| Forgetting dielectric effect on capacitance | Dielectric always increases capacitance by factor K (dielectric constant) |
| Using wrong energy formula | Use U = ½CV² when V is given, U = ½Q²/C when Q is given, U = ½QV for either |
| Not applying superposition for multiple charges | Always add potentials algebraically - they're scalars, not vectors |
| Confusing equipotential surfaces with field lines | Equipotential surfaces are always perpendicular to electric field lines |
| Wrong application of conductor properties | Inside conductor: E = 0, V = constant. At surface: E ⊥ surface |
Comprehensive Cheat Sheet for Revision
+🎯 THE ULTIMATE one-stop reference for your exam! This comprehensive cheat sheet contains everything you need for last-minute revision. Master this section and you're ready for any exam!
📊 Fundamental Constants & Values
🔄 Unit Conversions & Prefixes
⚡ Formula Quick Reference by Topic
Potential Formulas
Capacitor Formulas
Energy Formulas
🚀 Problem-Solving Shortcuts & Memory Aids
Parallel = same Potential, different Charges"
(E = -dV/dx)"
inCreases Capacitance"
½CV², ½QV, ½Q²/C"
