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...