Step 1: The nuclear density \( \rho \) is given by: \[ \rho = \frac{{Mass}}{{Volume}} = \frac{A}{\frac{4}{3} \pi R^3} \] where \( A \) is the mass number, and \( R \) is the radius of the nucleus.
The radius of the nucleus is related to the mass number \( A \) by the empirical relation: \[ R \propto A^{1/3} \]
Step 2: Therefore, the density is given by: \[ \rho \propto \frac{A}{R^3} \propto \frac{A}{(A^{1/3})^3} = \frac{A}{A} = 1 \]
Step 3: Hence, the ratio of the nuclear densities of the two nuclei will be \( 1:1 \).
A small bob A of mass m is attached to a massless rigid rod of length 1 m pivoted at point P and kept at an angle of 60° with vertical. At 1 m below P, bob B is kept on a smooth surface. If bob B just manages to complete the circular path of radius R after being hit elastically by A, then radius R is_______ m :