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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

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. R. S. Ex- E o 1 d E OC el. 1 d (A) P5; Q3, 4; (B) P5; (C) P 5; (D) P4; Q 3; Q 3; Q 2, 3; -> R-1; R 1,4; R 1, 2; R 1; S 2 S 2 S 4 S 5 LIST-II 1. 2. 3. 4. 5. A point charge Q at the origin A small dipole with point charges Q at (0, 0, 0) and-Q at (0, 0, -(). Take 20 < < d An infinite line charge coincident with the x-axis, with uniform linear charge density Two infinite wires carrying uniform linear charge density parallel to the x- axis. The one along (y=0, z =) has a charge density +2 and the one along (y = 0, z = () has a charge density -. Take 20 < < d Infinite plane charge coincident with the xy-plane with uniform surface charge density

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