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Four point size dense bodies of same mass are attached at four corners of a light square frame . Identify the decreasing order of their moments of inertia about following axes .
I) Passing through any side
II) Passing through opposite corners III) `bot^(r)` bisector of any side
(IV) `bot^(r)` to the plane and passing through any corner

A

III,IV,I,II

B

IV,III,I,II

C

III,II,IV,I

D

IV,III,II,I

Text Solution

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To determine the decreasing order of the moments of inertia of four point masses located at the corners of a square frame about various axes, we will calculate the moments of inertia for each case step by step. ### Given: - Four point masses, each of mass \( m \), are located at the corners of a square frame. - The side length of the square frame is assumed to be \( 2a \). ### Moments of Inertia Calculations: #### I) Moment of Inertia about an axis passing through any side (I1): - For this axis, only the two masses that are not on the axis contribute to the moment of inertia. - The distance of each of these two masses from the axis is \( a \) (half the side length). - Thus, the moment of inertia \( I_1 \) is given by: \[ I_1 = m \cdot a^2 + m \cdot a^2 = 2m \cdot a^2 \] #### II) Moment of Inertia about an axis passing through opposite corners (I2): - For this axis, the two masses at the corners through which the axis passes do not contribute (distance = 0). - The distance of the other two masses from the axis is the diagonal distance. - The diagonal length \( d \) is calculated as: \[ d = \sqrt{(2a)^2 + (2a)^2} = \sqrt{8a^2} = 2\sqrt{2}a \] - The distance of each mass from the axis is \( \frac{d}{2} = \sqrt{2}a \). - Thus, the moment of inertia \( I_2 \) is given by: \[ I_2 = m \left(\sqrt{2}a\right)^2 + m \left(\sqrt{2}a\right)^2 = 2m \cdot 2a^2 = 4m \cdot a^2 \] #### III) Moment of Inertia about the bisector of any side (I3): - The axis bisects the side, so the distance of the two masses on the opposite corners is \( \sqrt{(a^2 + a^2)} = \sqrt{2}a \). - Thus, the moment of inertia \( I_3 \) is given by: \[ I_3 = m \left(\sqrt{2}a\right)^2 + m \left(\sqrt{2}a\right)^2 = 2m \cdot 2a^2 = 4m \cdot a^2 \] #### IV) Moment of Inertia about an axis perpendicular to the plane and passing through any corner (I4): - The distance from the axis to each of the other three masses is \( 2a \) (the height from the corner to the plane). - Thus, the moment of inertia \( I_4 \) is given by: \[ I_4 = m(2a)^2 + m(2a)^2 + m(2a)^2 = 3m \cdot 4a^2 = 12m \cdot a^2 \] ### Summary of Moments of Inertia: - \( I_1 = 2ma^2 \) - \( I_2 = 4ma^2 \) - \( I_3 = 4ma^2 \) - \( I_4 = 12ma^2 \) ### Decreasing Order: Now we can arrange the moments of inertia in decreasing order: 1. \( I_4 = 12ma^2 \) 2. \( I_2 = 4ma^2 \) 3. \( I_3 = 4ma^2 \) 4. \( I_1 = 2ma^2 \) Thus, the decreasing order of the moments of inertia is: \[ I_4 > I_2 = I_3 > I_1 \]
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