Given:
- Electric field at point \( P \) on the axial line: \( E_P = E = \frac{2Kp}{r^3} \)
- Electric field at point \( R \) on the equatorial line: \( E_R = \frac{Kp}{(2r)^3} \), where:
- \( K \) is the Coulomb constant,
- \( p \) is the dipole moment,
- \( r \) is the distance from the dipole center to the point of observation.
Step 1: Calculate the Electric Field at \( R \)
The electric field at point \( R \) on the equatorial line is given by:
\[ E_R = \frac{Kp}{(2r)^3}. \]
Simplify \( (2r)^3 \):
\[ E_R = \frac{Kp}{8r^3}. \]
Step 2: Compare the Electric Fields
The electric field at \( P \) on the axial line is:
\[ E_P = \frac{2Kp}{r^3}. \]
The electric field at \( R \) is related to \( E_P \) as:
\[ E_R = \frac{E_P}{x}. \]
Substitute \( E_P = \frac{2Kp}{r^3} \) and \( E_R = \frac{Kp}{8r^3} \):
\[ \frac{Kp}{8r^3} = \frac{2Kp}{xr^3}. \]
Step 3: Solve for \( x \)
Simplify the equation:
\[ \frac{Kp}{8r^3} = \frac{2Kp}{xr^3}. \]
Cancel \( Kp \) and \( r^3 \) (as they are non-zero):
\[ \frac{1}{8} = \frac{2}{x}. \]
Rearrange to solve for \( x \):
\[ x = 2 \times 8 = 16. \]
Thus, the value of \( x \) is 16.
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below:
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