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 \( \frac{r_2}{r_1} = \frac{48000}{12000} = 4 \). \[ T_2 = 3 \times (4)^{3/2} = 3 \times (\sqrt{4})^3 = 3 \times (2)^3 = 3 \times 8 = 24 \text{ hours} \]
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 
