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:
Let's match the quantities in LIST-I with their corresponding dimensional formulas in LIST-II. Understanding the quantities and their respective dimensional formulas is essential in solving this type of question.
The gravitational constant \(G\) is used in Newton's law of universal gravitation: \(F = \frac{G \cdot m_1 \cdot m_2}{r^2}\), where \(F\) is the gravitational force. The dimensional formula for \(G\) can be derived by rearranging the formula: \(G = \frac{F \cdot r^2}{m_1 \cdot m_2}\). Thus, its dimensional formula is \([M^{-1}L^3T^{-2}]\).
This is the energy due to position in a gravitational field, given by \(U = m \cdot g \cdot h\). Here, \(m\) is mass, \(g\) is acceleration due to gravity, and \(h\) is height. So, its dimensional formula is \([ML^2T^{-2}]\).
The gravitational potential at a point is defined as the work done per unit mass to bring a mass from infinity to that point: \(V = \frac{U}{m} = \frac{m \cdot g \cdot h}{m} = g \cdot h\). Its dimensional formula can be derived as \([L^2T^{-2}]\).
The acceleration due to gravity \(g\) is the acceleration experienced by an object due to the gravitational force. Its dimensional formula is derived from \(F = m \cdot g\), leading to \(g = \frac{F}{m}\). Hence, its dimensional formula is \([LT^{-2}]\).
By matching the descriptions and dimensional formulas, we get the correct answer: A-IV, B-III, C-II, D-I.
(A) \( G = \frac{Fr^2}{m^2} \) \( [G] = \frac{[MLT^{-2}][L^2]}{[M^2]} = [M^{-1}L^3T^{-2}] \) (IV)
(B) P.E. = mgh = \( [MLT^{-2}L] = [ML^2T^{-2}] \) (III)
(C) Gravitational Potential = \( \frac{GM}{r} \) \( [M^{-1}L^3T^{-2}] \frac{[M]}{[L]} = [M^0L^2T^{-2}] = [L^2T^{-2}] \) (II)
(D) Acceleration due to gravity = \( \frac{GM}{r^2} \) \( [M^{-1}L^3T^{-2}] \frac{[M]}{[L^2]} = [M^0LT^{-2}] = [LT^{-2}] \) (I)
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: 
An organic compound (X) with molecular formula $\mathrm{C}_{3} \mathrm{H}_{6} \mathrm{O}$ is not readily oxidised. On reduction it gives $\left(\mathrm{C}_{3} \mathrm{H}_{8} \mathrm{O}(\mathrm{Y})\right.$ which reacts with HBr to give a bromide (Z) which is converted to Grignard reagent. This Grignard reagent on reaction with (X) followed by hydrolysis give 2,3-dimethylbutan-2-ol. Compounds (X), (Y) and (Z) respectively are: