A frictionless pulley has a rope of negligible mass passing over it. B

A frictionless pulley has a rope of negligible mass passing over it. Blocks of mass 15 kg and 5 kg are attached at the two ends of the rope and held stationary. When the masses are released to move freely, their speed in m s-1, after the rope has slipped by 0.25 m over the pulley, is closest to :
(take g = 10.0 m s-2)

5.0
2.2
1.6
1.2
This question was previously asked in
UPSC Geoscientist – 2024
Correct Answer: C
– This problem can be solved using the conservation of mechanical energy, as the pulley is frictionless and the rope has negligible mass (ideal Atwood machine).
– Let the initial height of the 15 kg mass be $y_1$ and the 5 kg mass be $y_2$. When the rope slips by 0.25 m, the 15 kg mass moves down by 0.25 m (new height $y_1 – 0.25$) and the 5 kg mass moves up by 0.25 m (new height $y_2 + 0.25$).
– The initial potential energy (PE) can be set relative to the initial positions. $\text{PE}_{initial} = m_1 g y_1 + m_2 g y_2$.
– The final potential energy is $\text{PE}_{final} = m_1 g (y_1 – 0.25) + m_2 g (y_2 + 0.25) = m_1 g y_1 – 0.25 m_1 g + m_2 g y_2 + 0.25 m_2 g$.
– The change in potential energy is $\Delta \text{PE} = \text{PE}_{final} – \text{PE}_{initial} = -0.25 m_1 g + 0.25 m_2 g = 0.25 g (m_2 – m_1)$.
– Given $m_1 = 15$ kg, $m_2 = 5$ kg, and $g = 10.0$ m/s², $\Delta \text{PE} = 0.25 \times 10 \times (5 – 15) = 2.5 \times (-10) = -25$ J. The system loses 25 J of potential energy.
– The initial kinetic energy (KE) is zero as the masses are held stationary. $\text{KE}_{initial} = 0$.
– Let $v$ be the speed of the masses after moving 0.25 m. Both masses move with the same speed. The final kinetic energy is $\text{KE}_{final} = \frac{1}{2} m_1 v^2 + \frac{1}{2} m_2 v^2 = \frac{1}{2} (m_1 + m_2) v^2$.
– $\text{KE}_{final} = \frac{1}{2} (15 + 5) v^2 = \frac{1}{2} (20) v^2 = 10 v^2$.
– By the conservation of mechanical energy, $\Delta \text{KE} + \Delta \text{PE} = 0$.
– $(10 v^2 – 0) + (-25) = 0$.
– $10 v^2 = 25$.
– $v^2 = \frac{25}{10} = 2.5$.
– $v = \sqrt{2.5}$ m/s.
– Calculating the value: $\sqrt{2.5} \approx 1.581$ m/s.
– Comparing with the options, 1.6 m/s is the closest value.
The motion of the masses in an Atwood machine is a classic physics problem demonstrating Newton’s laws or conservation of energy. Assuming an ideal setup (frictionless pulley, massless rope), energy is conserved, meaning the decrease in potential energy of the heavier mass going down is converted into the increase in potential energy of the lighter mass going up and the kinetic energy of both masses.