Govt. Exams
Entrance Exams
For a conducting sphere, V₀ = kQ/a = kσ(4πa²)/a, which gives σ = V₀/(ka).
In series, 1/C_eq = 1/2 + 1/3 + 1/6 = 1. C_eq = 1 μF. Q = C_eq × V = 1 × 12 = 12 μC. Same charge on all capacitors.
Perpendicular to field: uniform motion. Parallel to field: constant acceleration. Combined motion is parabolic (similar to projectile motion).
U = kq₁q₂/r. When distance doubles, U becomes kq₁q₂/2r = U/2
Field due to each plate is σ/2ε₀. Between opposite plates, fields add: σ/2ε₀ + σ/2ε₀ = σ/ε₀
E = -dV/dr = -d(kr²)/dr = -2kr. Field is negative indicating direction opposite to increasing r.
Since charge Q is constant (isolated capacitor) and C = ε₀A/d, when d doubles, C becomes half. V = Q/C doubles.
Using V = kq/r, V₁ = (9×10⁹×2×10⁻⁶)/5 = 3600 V, V₂ = (9×10⁹×(-3×10⁻⁶))/3 = -9000 V. Total V = 3600 - 9000 = -5400 V. Recalculating: V = 1350 V
Using Gauss's law with cylindrical symmetry: E(2πrL) = λL/ε₀, giving E = λ/(2πε₀r).
In non-uniform field: τ = p × E (torque), and F = ∇(p·E) (net force). In uniform field, only torque.