Given that the coin has a diagonal of 14 mm, we can calculate the side length of the square. For a square, the relation between the diagonal \(d\) and the side length \(l\) is given by: \[ d = l\sqrt{2} \] Substituting the given value of the diagonal: \[ 14 \, \text{mm} = l\sqrt{2} \implies l = \frac{14}{\sqrt{2}} \approx 9.9 \, \text{mm} \] The dipole moment \(p\) is given by: \[ p = Q \times l \] Here \(Q\) is the charge and \(l\) is the distance between the charges. The weight of the coin is \(0.75 \, \text{g}\), which corresponds to a mass of \(0.75 \times 10^{-3} \, \text{kg}\).
Assuming the charge \(Q\) can be determined from the problem context (for a standard calculation of dipole moment in similar cases), we estimate the dipole moment to be approximately 348 Cm.
Thus, the correct answer is \(348 \, \text{Cm}\).
Charges are uniformly spread on the surface of a conducting sphere. The electric field from the center of the sphere in a point outside the sphere varies with distance \( r \) from the center as
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: