This problem requires the calculation of the moment of inertia for a three-mass system positioned at the midpoints of an equilateral triangle's sides. The rotation axis is defined as passing through the triangle's centroid and being perpendicular to its plane.
The methodology relies on the formula for the moment of inertia of discrete point masses and the geometric characteristics of an equilateral triangle.
Step 1: Identify the given parameters.
Step 2: Determine the distance of each mass from the axis of rotation.
The axis of rotation passes through the centroid and is perpendicular to the triangle's plane. The masses are located at the midpoints of the sides. Therefore, the perpendicular distance of each mass from the axis is its distance from the centroid within the triangle's plane.
First, calculate the median length (\(h\)) of the triangle:
\[h = \frac{\sqrt{3}}{2}s = \frac{\sqrt{3}}{2}(2 \, \text{m}) = \sqrt{3} \, \text{m}\]The centroid of an equilateral triangle is equidistant from the midpoints of its sides. This distance (\(r\)) is one-third the median length:
\[r = \frac{1}{3}h = \frac{\sqrt{3}}{3} \, \text{m} = \frac{1}{\sqrt{3}} \, \text{m}\]Consequently, all three masses are at an identical perpendicular distance \(r = \frac{1}{\sqrt{3}} \, \text{m}\) from the axis of rotation.
Step 3: Apply the moment of inertia formula.
The total moment of inertia (\(I\)) is the sum of the individual moments of inertia of the three masses:
\[I = m_1 r^2 + m_2 r^2 + m_3 r^2\]As the distance \(r\) is constant for all masses, we can factor out \(r^2\):
\[I = (m_1 + m_2 + m_3) r^2\]Step 4: Substitute the values and compute the final result.
Calculate the total mass of the system:
\[M = m_1 + m_2 + m_3 = 2 \, \text{kg} + 4 \, \text{kg} + 6 \, \text{kg} = 12 \, \text{kg}\]Calculate the square of the distance \(r\):
\[r^2 = \left(\frac{1}{\sqrt{3}}\right)^2 = \frac{1}{3} \, \text{m}^2\]Compute the total moment of inertia:
\[I = (12 \, \text{kg}) \times \left(\frac{1}{3} \, \text{m}^2\right)\]\[I = 4 \, \text{kg} \, \text{m}^2\]The moment of inertia of the system about the specified axis is 4 kg m².
For a uniform rectangular sheet shown in the figure, the ratio of moments of inertia about the axes perpendicular to the sheet and passing through \( O \) (the center of mass) and \( O' \) (corner point) is:
