Step 1: Formula for the time period of a simple pendulum.
\[
T = 2\pi \sqrt{\frac{L}{g}}
\]
where \( g \) is the acceleration due to gravity.
Step 2: Relation of \( g \) with planet’s mass and radius.
\[
g = \frac{GM}{R^2}.
\]
Let \( g_E \) be the acceleration due to gravity on Earth and \( g_P \) on the new planet.
Given: \[ M_P = 4M_E, \quad R_P = 2R_E. \] Thus, \[ g_P = \frac{G M_P}{R_P^2} = \frac{G(4M_E)}{(2R_E)^2} = \frac{4GM_E}{4R_E^2} = g_E. \]
Step 3: Compare time periods.
Since \( g_P = g_E \),
\[
T_P = 2\pi \sqrt{\frac{L}{g_P}} = 2\pi \sqrt{\frac{L}{g_E}} = T_E.
\]
Hence, **time period remains the same.**
Step 4: Analyze statements.
- Assertion (A): “Time period remains same” → ✅ True (since \( g_P = g_E \)).
- Reason (R): “Mass of the pendulum remains unchanged” → although true as a physical fact, **it is not the reason** why the time period remains same — time period depends on \( g \), not on the pendulum’s mass.
\[ \boxed{\text{(A) is true but (R) is false.}} \]
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 

Which of the following best represents the temperature versus heat supplied graph for water, in the range of \(-20^\circ\text{C}\) to \(120^\circ\text{C}\)? 