The capacitance without the dielectric is:
\[C = \frac{A \epsilon_0}{d}.\]
With the dielectric inserted:
\[C = \frac{A \epsilon_0}{0.2 + \frac{d}{k}}.\]
Equating the capacitances:
\[\frac{A \epsilon_0}{0.6} = \frac{A \epsilon_0}{0.2 + \frac{0.6}{k}}.\]
Cancel \(A \epsilon_0\):
\[0.6 = 0.2 + \frac{0.6}{k}.\]
Rearranging:
\[0.6 - 0.2 = \frac{0.6}{k} \implies 0.4 = \frac{0.6}{k}.\]
Solving for \(k\):
\[k = \frac{0.6}{0.4} = \frac{3}{2} = 1.50.\]
Thus, the dielectric constant of the slab is:
\[k = 1.50.\]
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:
A point charge $ +q $ is placed at the origin. A second point charge $ +9q $ is placed at $ (d, 0, 0) $ in Cartesian coordinate system. The point in between them where the electric field vanishes is:
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: