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The moment of inertia of a disc of mass ...

The moment of inertia of a disc of mass `M` and radius `R` about an axis. Which is tangential to sircumference of disc and parallel to its diameter is.

A

`(5)/(4)MR^(2)`

B

`(2)/(3)MR^(2)`

C

`(3)/(2)MR^(2)`

D

`(1)/(2)MR^(2)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the moment of inertia of a disc of mass \( M \) and radius \( R \) about an axis that is tangential to the circumference of the disc and parallel to its diameter, we can follow these steps: ### Step 1: Understand the Problem We need to calculate the moment of inertia of a disc about a specific axis. The axis is tangential to the circumference of the disc and parallel to its diameter. ### Step 2: Moment of Inertia about the Center The moment of inertia of a disc about an axis passing through its center and perpendicular to its plane is given by the formula: \[ I_{CM} = \frac{1}{2} M R^2 \] ### Step 3: Use the Perpendicular Axis Theorem According to the perpendicular axis theorem, for a planar body, the moment of inertia about an axis perpendicular to the plane (z-axis) is equal to the sum of the moments of inertia about two perpendicular axes (x-axis and y-axis) lying in the plane of the body: \[ I_Z = I_X + I_Y \] For a disc, since the moment of inertia about the x-axis and y-axis is the same (due to symmetry): \[ I_X = I_Y = I_D \] Thus, \[ I_Z = 2 I_D \] From the earlier step, we know: \[ I_Z = \frac{1}{2} M R^2 \] So, \[ 2 I_D = \frac{1}{2} M R^2 \implies I_D = \frac{1}{4} M R^2 \] ### Step 4: Apply the Parallel Axis Theorem Now, we need to find the moment of inertia about the tangential axis. We can use the parallel axis theorem, which states: \[ I = I_{CM} + Md^2 \] where \( d \) is the distance from the center of mass axis to the new axis. In this case, \( d = R \) (the radius of the disc). ### Step 5: Calculate the Moment of Inertia about the Tangential Axis Substituting the values we have: \[ I = I_D + M R^2 \] Substituting \( I_D = \frac{1}{4} M R^2 \): \[ I = \frac{1}{4} M R^2 + M R^2 \] \[ I = \frac{1}{4} M R^2 + \frac{4}{4} M R^2 = \frac{5}{4} M R^2 \] ### Final Answer Thus, the moment of inertia of the disc about the tangential axis is: \[ I = \frac{5}{4} M R^2 \]
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