2.Electrotatics Solutions
2. ELECTROSTATICS 14.1 (D) R = = 8 N 8N 8N 14.2 (B) We can consider all the charge inside the sphere to be concentrated on the centre of sphere Consider an elementry shell of radius x and thickness dx. E = K dq r 2 K 4 x2dx(ax) = r2 = r 2 4 0 14.3 (A) We have centripetal force equation q 2k mv2 r = so v = 1 r Now, T = 2r v = where, k = 40 –→ → –→ ˆi q (x x ) 14.4 (A) Wnet = q E.d where E = 20 = 20 1 2 14.5 (A) Electric field between the two cylinders = 2kq 2k r \ Force on charge q = r This force is centrepetal force 2kq \ r = mv2 r \ v = = 14.6 (A) V = V1 + V2 + V3 = 1 Q 1 2Q 1 3Q = 1 2Q 4 R 4 R 4 R 4 R 0 0 0 0 14.7 (B) dV = v → → E.dr = 1 (–2x3ˆi ) . (dx ˆi dy ˆj dzkˆ) = 2x3 dx Þ dV = 0 (2x3 ) 103 dx Þ V = – 7.5 × 10...