Step 1: Start with Kepler’s Third Law \[ T \propto \sqrt{\dfrac{a^3}{GM}} \] But \( g = \dfrac{GM}{R^2} \Rightarrow GM = gR^2 \)
Step 2: Substitute \( GM \) in the original formula \[ T \propto \sqrt{\dfrac{a^3}{gR^2}} = a^{3/2}g^{-1/2}R^{-1} \] Step 3: Compare with given form Given: \[ T \propto a^{3/2}g^xR^y \Rightarrow x = -\dfrac{1}{2}, \quad y = -1 \]
Match the LIST-I with LIST-II
\[ \begin{array}{|l|l|} \hline \text{LIST-I} & \text{LIST-II} \\ \hline \text{A. Gravitational constant} & \text{I. } [LT^{-2}] \\ \hline \text{B. Gravitational potential energy} & \text{II. } [L^2T^{-2}] \\ \hline \text{C. Gravitational potential} & \text{III. } [ML^2T^{-2}] \\ \hline \text{D. Acceleration due to gravity} & \text{IV. } [M^{-1}L^3T^{-2}] \\ \hline \end{array} \]
Choose the correct answer from the options given below:
A small point of mass \(m\) is placed at a distance \(2R\) from the center \(O\) of a big uniform solid sphere of mass \(M\) and radius \(R\). The gravitational force on \(m\) due to \(M\) is \(F_1\). A spherical part of radius \(R/3\) is removed from the big sphere as shown in the figure, and the gravitational force on \(m\) due to the remaining part of \(M\) is found to be \(F_2\). The value of the ratio \( F_1 : F_2 \) is: 