The electric field E is measured at a point P(0,0,d) generated due to various charge distributions and the dependence of E on d is found to be different for different charge distributions.
Column-II describes different electric charge distributions, along with their locations. Match the functions in column-I with the related charge distributions in column-II.
column -I | column-II |
(A) E is independent of d | (P) A point charge Q at the origin |
(B) E∝1d | (Q) A small dipole with point charges Q at (0,0,l) and −Q at (0,0,−l). Take 2l<<<d. |
(C) E∝1d2 | (R) An infinite line charge coincident with the x- axis, with uniform linear charge density λ |
(D) E∝1d3 | (S) Two infinite wire carrying uniform linear charge density parallel to the x-axis. The one along (y=0,z=l) has a charge density λ and the another along (y=0,z=−l) has a charge density −λ. Take 2l<<d. |
(T) Infinite plane charge coincident with the xy-plane with uniform surface charge density. |