We are given the relation:
\[
\frac{A \varepsilon_0}{d} = \frac{A \varepsilon_0}{(0.2 + \frac{d}{k})}
\]
Step 1: Simplify the equation
By canceling out \( A \varepsilon_0 \) on both sides, we get:
\[
\frac{1}{d} = \frac{1}{0.2 + \frac{d}{k}}
\]
Multiplying both sides by \( d(0.2 + \frac{d}{k}) \), we have:
\[
0.6 = 0.2 + \frac{0.6}{k}
\]
Step 2: Solving for \( k \)
Rearranging the equation:
\[
0.6 - 0.2 = \frac{0.6}{k}
\]
\[
0.4 = \frac{0.6}{k}
\]
\[
k = \frac{0.6}{0.4} = \frac{3}{2}
\]
Final Answer:
\[
k = \frac{3}{2}
\]
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:
\[k = 1.50.\]
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :
