Class 12 · Chapter
Electrostatic Potential & Capacitance
18 topics · 18 interactive simulations
🎚️
Potential due to Point Charge
V = kq/r. Drag a probe and read live potential with full heatmap.
Foundation9 minlive
📊
V & E vs Distance
1/r and 1/r² overlaid — confirm E = −dV/dr.
Moderate8 minlive
🗺️
Equipotential Surfaces
Banded contours for single charge, dipole, two-+. Always perpendicular to E.
Moderate10 minlive
↔️
E = −dV/dx
Linear V → constant E. Graphs side-by-side.
Moderate8 minlive
🧲
Potential of Dipole
V = (kp cosθ)/r². Zero on equatorial plane, max on axis.
Advanced10 minlive
🚶
Work Moving a Charge
W = q(V_B − V_A). Independent of path between two equipotentials.
Moderate9 minlive
🔋
Parallel-Plate Capacitor
C = ε₀A/d. Animated dots show field. Live Q, E, U.
Foundation10 minlive
🧊
Effect of Dielectric
C' = κC₀. Toggle V-fixed (Q grows) vs Q-fixed (V drops).
Moderate10 minlive
🔋
Energy Stored in Capacitor
U = ½CV². Visualized as triangular area under Q-V curve.
Moderate8 minlive
📈
RC Charging
q(t) = CV(1 − e^(−t/τ)). Watch the curve build with τ marked.
Advanced10 minlive
📉
RC Discharging
q(t) = Q₀ e^(−t/τ). 37% remaining at τ marked clearly.
Advanced10 minlive
🔗
Capacitors in Series
1/C_eq = Σ 1/Cᵢ. Same Q. Voltage divides inversely with C.
Moderate9 minlive
🔗
Capacitors in Parallel
C_eq = ΣCᵢ. Same V. Charge splits proportionally to C.
Moderate9 minlive
📻
Variable (Air-Gang) Capacitor
C ∝ |cosθ|. Rotate the shaft to tune from radio receiver-style sweep.
Advanced9 minlive
📥
Dielectric Slab Insertion
Slab gets pulled in by force F = ε₀bV²(κ−1)/(2d).
Advanced10 minlive
🧲
Force Between Plates
F = Q²/(2ε₀A). Always attractive (opposite sign plates).
Advanced9 minlive
⚡
Dielectric Breakdown
Each dielectric has a breakdown E_max. Above it, the dielectric arcs.
Advanced9 minlive
🔌
Battery Removal Case
Insert dielectric with battery on/off — different physics. Compare side-by-side.
Advanced10 minlive