The force between two point charges \(q_1\) and \(q_2\) separated by a distance \(r\) in a vacuum is given by Coulomb’s law:
\[ F = \frac{1}{4 \pi \epsilon_0} \frac{q_1 q_2}{r^2}, \]
where \(\epsilon_0\) is the permittivity of free space.
In a medium with dielectric constant \(K\), the permittivity changes from \(\epsilon_0\) to \(K \epsilon_0\). This reduces the effective force between the charges by a factor of \(K\). Thus, the force in the medium, if the distance remained \(r\), would be:
\[ F_{\text{medium}} = \frac{1}{4 \pi K \epsilon_0} \frac{q_1 q_2}{r^2} = \frac{F}{K}. \]
For \(K = 5\), this becomes:
\[ F_{\text{medium}} = \frac{F}{5}. \]
Now, since the distance between the charges is reduced to \(\frac{r}{5}\), we need to adjust for this change. Coulomb’s force varies inversely with the square of the distance, so reducing the distance by a factor of \(\frac{1}{5}\) increases the force by a factor of \(\left(\frac{1}{5}\right)^{-2} = 25\).
Combining both effects (the dielectric and the reduced distance), the modified force \(F'\) in the medium is:
\[ F' = \frac{F}{5} \times 25 = 5F. \]
Thus, the force between the charges in the medium, with the distance changed to \(\frac{r}{5}\), is increased by a factor of 5 compared to the original force in a vacuum. Therefore, the answer is: \[ 5F. \]
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).