Three identical spheres, each with mass \(2M\), are positioned at the vertices of a right-angled triangle with sides measuring 4 m. The origin \((0, 0)\) is set at the intersection of the two sides forming the right angle. The position vectors for these masses are:
The formula for the position vector of the center of mass is:
\[ r_{\text{com}} = \frac{m_1 r_1 + m_2 r_2 + m_3 r_3}{m_1 + m_2 + m_3} \]
Substituting the given values yields:
\[ r_{\text{com}} = \frac{2M \times (0, 0) + 2M \times (4, 0) + 2M \times (0, 4)}{6M} = \left(\frac{4}{3}, \frac{4}{3}\right) \]
The magnitude of \(r_{\text{com}}\) is calculated as:
\[ |r_{\text{com}}| = \sqrt{\left(\frac{4}{3}\right)^2 + \left(\frac{4}{3}\right)^2} = \sqrt{\frac{16}{9} + \frac{16}{9}} = \sqrt{\frac{32}{9}} = \frac{4\sqrt{2}}{3} \]
Therefore, \(x = 3\).
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 