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. List-I contains different
relations between \(E\) and \(d\). List-II describes different electric charge
distributions, along with their locations. Match the functions in List-I with
the related charge distributions in List-II.
LIST-I
P. \(E\) is independent of \(d\)
Q. \(E \propto \frac{1}{d}\)
R. \(E \propto \frac{1}{d^{2}}\)
S. \(E \propto \frac{1}{d^{3}}\)
LIST-II
1\. A point charge \(Q\) at the origin
2\. A small dipole with point charges \(Q\) at \((0,0, l)\) and \(-Q\) at \((0,0,-l)\)
Take \(2 l \ll d\)
3\. An infinite line charge coincident with the \(x\) -axis, with uniform linear
charge density \(\lambda\)
4\. Two infinite wires carrying uniform linear charge density parallel to the
\(x\) - axis. The one along \((y=0, z=l)\) has a charge density \(+\lambda\) and the
one along \((y=0, z=-l)\) has a charge density \(-\lambda\). Take \(2 l \ll d\)
5\. Infinite plane charge coincident with the \(x y\) -plane with uniform
surface charge density