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 \(348 \, \text{Cm}\).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: