Step 1: State Kepler's Third Law of planetary motion. For objects orbiting the same central body, the square of the orbital period (\(T\)) is directly proportional to the cube of the semi-major axis of its orbit. For a circular orbit, this is the radius (\(r\)). \[ \frac{T^2}{r^3} = \text{constant} \]
Step 2: Set up a ratio for the two satellites. Let \(T_1, r_1\) be the period and radius for the first satellite, and \(T_2, r_2\) for the second. \[ \frac{T_1^2}{r_1^3} = \frac{T_2^2}{r_2^3} \]
Step 3: Rearrange the formula to solve for the unknown period, \(T_2\). \[ T_2^2 = T_1^2 \left( \frac{r_2}{r_1} \right)^3 \] \[ T_2 = T_1 \left( \frac{r_2}{r_1} \right)^{3/2} \]
Step 4: Substitute the given values and calculate \(T_2\). - \( T_1 = 3 \) hours - \( r_1 = 12000 \) km - \( r_2 = 48000 \) km The ratio of the radii is \( \frac{r_2}{r_1} = \frac{48000}{12000} = 4 \). \[ T_2 = 3 \times (4)^{3/2} = 3 \times (\sqrt{4})^3 = 3 \times (2)^3 = 3 \times 8 = 24 \text{ hours} \]
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: 
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: