A planet has double the mass of the earth. Its average density is equal to that of the earth. An object weighing W on earth will weigh on that planet:
1
(2)\(^{\frac{1}{3}}\)
(2)\(^{-\frac{1}{3}}\)
2
The correct answer is option (B): \((2) ^{\frac{1}{3}}\)

Let \( M_e, R_e, \) and \( \rho_e \) be the mass, radius, and average density of Earth, respectively. Let \( M_p, R_p, \) and \( \rho_p \) be the mass, radius, and average density of the planet, respectively. Given that \( M_p = 2M_e \) and \( \rho_p = \rho_e \). Density is defined as mass divided by volume: \( \rho = \frac{M}{V} \). Assuming spherical shapes, \( V = \frac{4}{3} \pi R^3 \). Thus:
\( \rho_e = \frac{M_e}{\frac{4}{3}\pi R_e^3} \) and \( \rho_p = \frac{M_p}{\frac{4}{3}\pi R_p^3} \)
Since \( \rho_e = \rho_p \):
\( \frac{M_e}{R_e^3} = \frac{M_p}{R_p^3} \)
\( \frac{M_e}{R_e^3} = \frac{2M_e}{R_p^3} \)
\( R_p^3 = 2R_e^3 \implies R_p = 2^{1/3} R_e \)
Weight (W) is given by \( W = mg \), where \( m \) is the mass of the object and \( g \) is the acceleration due to gravity.
The acceleration due to gravity (g) is given by:
\( g = \frac{GM}{R^2} \)
where \( G \) is the gravitational constant, \( M \) is the mass of the planet, and \( R \) is the radius. Let \( g_e \) and \( g_p \) be the acceleration due to gravity on Earth and the planet, respectively.
\( \frac{g_e}{g_p} = \frac{M_e / R_e^2}{M_p / R_p^2} = \frac{M_e}{R_e^2} \times \frac{R_p^2}{M_p} = \frac{M_e}{R_e^2} \times \frac{(2^{1/3} R_e)^2}{2M_e} = \frac{2^{2/3}}{2} = 2^{-1/3} \)
\( g_p = 2^{1/3} g_e \)
Since the mass of the object remains constant, the weight on the planet (\( W_p \)) is:
\( W_p = mg_p = m(2^{1/3} g_e) = 2^{1/3} (mg_e) = 2^{1/3} W \)
The object will weigh \( \mathbf{2^{1/3}W} \) on the planet (Option 1).
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:

Let \( a \in \mathbb{R} \) and \( A \) be a matrix of order \( 3 \times 3 \) such that \( \det(A) = -4 \) and \[ A + I = \begin{bmatrix} 1 & a & 1 \\ 2 & 1 & 0 \\ a & 1 & 2 \end{bmatrix} \] where \( I \) is the identity matrix of order \( 3 \times 3 \).
If \( \det\left( (a + 1) \cdot \text{adj}\left( (a - 1) A \right) \right) \) is \( 2^m 3^n \), \( m, n \in \{ 0, 1, 2, \dots, 20 \} \), then \( m + n \) is equal to:
In mechanics, the universal force of attraction acting between all matter is known as Gravity, also called gravitation, . It is the weakest known force in nature.
According to Newton’s law of gravitation, “Every particle in the universe attracts every other particle with a force whose magnitude is,
On combining equations (1) and (2) we get,
F ∝ M1M2/r2
F = G × [M1M2]/r2 . . . . (7)
Or, f(r) = GM1M2/r2
The dimension formula of G is [M-1L3T-2].