1. Center of Mass Movement Definition: The total displacement of the center of mass (\(\Delta X_\text{C.O.M.}\)) must be zero to preserve its position.
2. Center of Mass Condition Application: If \(m_2\) moves \(x\) cm toward the center of mass, the condition is:
\[ \Delta X_\text{C.O.M.} = \frac{m_1 \Delta x_1 + m_2 \Delta x_2}{m_1 + m_2}, \] with \(\Delta x_1 = 2 \, \text{cm}\) representing the movement of \(m_1\) and \(\Delta x_2 = -x \, \text{cm}\) representing the movement of \(m_2\).
3. Setting \(\Delta X_\text{C.O.M.}\) to Zero:
\[ 0 = \frac{3 \times 2 + 2 \times (-x)}{3 + 2}. \] Upon simplification,
\[ 6 - 2x = 0. \] This yields,
\[ x = 3 \, \text{cm}. \]
Answer: \(3 \, \text{cm}\)
The variation of density of a solid cylindrical rod of cross-sectional area \( a \) and length \( L \) is \( \rho=\rho_0 \frac{x^2}{L^2} \), where \( x \) is the distance from one end. The position of its centre of mass from \( x=0 \) is 