We are given that three particles of mass \( m \) are placed at the vertices of an equilateral triangle with side length \( l \). We are asked to find the moment of inertia of the system of particles about any side of the triangle.
Step 1: Moment of inertia formula. The moment of inertia of a system of point masses is given by: \[ I = \sum m_i r_i^2, \] where \( m_i \) is the mass of the \( i \)-th particle and \( r_i \) is the perpendicular distance from the axis of rotation.
Step 2: Geometry of the problem. The particles are placed at the vertices of an equilateral triangle. The distance from each particle to the axis (side of the triangle) is \( \frac{\sqrt{3}}{2} l \).
Step 3: Moment of inertia calculation. The moment of inertia of the two particles not on the axis is: \[ I = 2 \cdot m \cdot \left( \frac{\sqrt{3}}{2} l \right)^2 = 2 \cdot m \cdot \frac{3}{4} l^2 = \frac{3}{2} m l^2. \]
Step 4: Final answer. Thus, the moment of inertia is \( \frac{3}{4} m l^2 \), corresponding to Option 3.
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The range of the real valued function \( f(x) =\) \(\sin^{-1} \left( \frac{1 + x^2}{2x} \right)\) \(+ \cos^{-1} \left( \frac{2x}{1 + x^2} \right)\) is:
If \(3A = \begin{bmatrix} 1 & 2 & 2 \\[0.3em] 2 & 1 & -2 \\[0.3em] a & 2 & b \end{bmatrix}\) and \(AA^T = I\), then\(\frac{a}{b} + \frac{b}{a} =\):
\(\begin{vmatrix} a+b+2c & a & b \\[0.3em] c & b+c+2c & b \\[0.3em] c & a & c+a2b \end{vmatrix}\)