To solve this problem, we need to determine the position $x_0$ where a new mass $m_4$ = 4 is placed, given the changes in the center of mass. Initially, the center of mass $x_{cm,\text{initial}}$ of masses $m_1$, $m_2$, and $m_3$ is given as 1. We use the center of mass formula: \[ x_{cm} = \frac{\sum (m_i \cdot x_i)}{\sum m_i} \] For the initial setup with $m_1 = 1$, $m_2 = 2$, $m_3 = 3$, and their center at $x = 1$: \[ 1 = \frac{1 \cdot x_1 + 2 \cdot x_2 + 3 \cdot x_3}{6} \] Using $x_{cm,\text{initial}} = 1$, we derive: \[ 1 \cdot x_1 + 2 \cdot x_2 + 3 \cdot x_3 = 6 \] Now, when the additional mass $m_4 = 4$ is placed at $x = x_0$, the new center of mass $x_{cm,\text{new}}$ becomes 3: \[ 3 = \frac{6 + 4 \cdot x_0}{10} \] Solving for $x_0$: \[ 3 \cdot 10 = 6 + 4 \cdot x_0 \] \[ 30 = 6 + 4 \cdot x_0 \] \[ 24 = 4 \cdot x_0 \] \[ x_0 = \frac{24}{4} \] \[ x_0 = 6 \] Thus, the position of the new mass is \( x_0 = 6 \).
In order to achieve the static equilibrium of the see-saw about the fulcrum \( P \), shown in the figure, the weight of Box B should be _________ kg, if the weight of Box A is 50 kg.

A particle of mass 1kg, initially at rest, starts sliding down from the top of a frictionless inclined plane of angle \(\frac{𝜋}{6}\)\(\frac{\pi}{6}\) (as schematically shown in the figure). The magnitude of the torque on the particle about the point O after a time 2seconds is ______N-m. (Rounded off to nearest integer) 
(Take g = 10m/s2)

