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 A be a 3 × 3 matrix such that \(\text{det}(A) = 5\). If \(\text{det}(3 \, \text{adj}(2A)) = 2^{\alpha \cdot 3^{\beta} \cdot 5^{\gamma}}\), then \( (\alpha + \beta + \gamma) \) is equal to:
Let \( \alpha, \beta \) be the roots of the equation \( x^2 - ax - b = 0 \) with \( \text{Im}(\alpha) < \text{Im}(\beta) \). Let \( P_n = \alpha^n - \beta^n \). If \[ P_3 = -5\sqrt{7}, \quad P_4 = -3\sqrt{7}, \quad P_5 = 11\sqrt{7}, \quad P_6 = 45\sqrt{7}, \] then \( |\alpha^4 + \beta^4| \) is equal to: