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The moment of inertia of a uniform semic...

The moment of inertia of a uniform semicircular wire of mass m and radius r, about an axis passing through its centre of mass and perpendicular to its plane is `mr^(2)(-(k)/(pi^(2)))`. Find the value of k.

A

`(mr^(2))/(2)`

B

`mr^(2)`

C

`mr^(2)(1-(4)/(pi^(2)))`

D

`mr^(2)(1+(4)/(pi^(2)))`

Text Solution

AI Generated Solution

The correct Answer is:
To find the value of \( k \) in the moment of inertia of a uniform semicircular wire of mass \( m \) and radius \( r \) about an axis passing through its center of mass and perpendicular to its plane, we can follow these steps: ### Step 1: Understand the Geometry We have a semicircular wire with mass \( m \) and radius \( r \). The center of mass (COM) of the semicircular wire lies along the vertical axis at a distance \( d \) from the center of the semicircle. ### Step 2: Find the Distance to the Center of Mass The distance \( d \) of the center of mass from the center of the semicircle can be calculated using the formula: \[ d = \frac{2r}{\pi} \] ### Step 3: Apply the Parallel Axis Theorem To find the moment of inertia \( I_O \) about the axis through the center of mass, we can use the parallel axis theorem: \[ I_O = I_{CM} + m d^2 \] where \( I_{CM} \) is the moment of inertia about the center of mass, and \( m d^2 \) accounts for the shift in the axis. ### Step 4: Calculate the Moment of Inertia About the Center of Mass The moment of inertia \( I_{CM} \) of a semicircular wire about its center of mass is given by: \[ I_{CM} = \frac{1}{2} m r^2 \] ### Step 5: Substitute Values into the Parallel Axis Theorem Now substituting the values into the parallel axis theorem: \[ I_O = \frac{1}{2} m r^2 + m \left(\frac{2r}{\pi}\right)^2 \] Calculating \( m \left(\frac{2r}{\pi}\right)^2 \): \[ m \left(\frac{2r}{\pi}\right)^2 = m \cdot \frac{4r^2}{\pi^2} \] ### Step 6: Combine the Terms Now we combine the terms: \[ I_O = \frac{1}{2} m r^2 + \frac{4m r^2}{\pi^2} \] To combine these, we need a common denominator: \[ I_O = \frac{\pi^2}{2\pi^2} m r^2 + \frac{4m r^2}{\pi^2} = \frac{\pi^2 + 8}{2\pi^2} m r^2 \] ### Step 7: Express in the Required Form We need to express this in the form \( m r^2 \left(1 - \frac{k}{\pi^2}\right) \): \[ I_O = m r^2 \left( \frac{1}{2} + \frac{4}{\pi^2} \right) = m r^2 \left( 1 - \frac{4}{\pi^2} \right) \] ### Step 8: Identify \( k \) From the expression, we can see that: \[ 1 - \frac{k}{\pi^2} = \frac{1}{2} + \frac{4}{\pi^2} \] Thus, we can equate: \[ k = 4 \] ### Final Answer The value of \( k \) is \( 4 \). ---
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