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The radius of gyration of a uniform circ...

The radius of gyration of a uniform circular disc of radius `R`, about any diameter of the disc is

A

`K = R`

B

`K = R//2`

C

`K = 2 R`

D

none of these

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The correct Answer is:
To find the radius of gyration \( k \) of a uniform circular disc of radius \( R \) about any diameter of the disc, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Moment of Inertia**: The moment of inertia \( I \) of a uniform circular disc about an axis through its center and perpendicular to its plane is given by the formula: \[ I = \frac{1}{2} m R^2 \] where \( m \) is the mass of the disc and \( R \) is its radius. 2. **Use the Perpendicular Axis Theorem**: The perpendicular axis theorem states that for a planar body, the moment of inertia about an axis perpendicular to the plane is the sum of the moments of inertia about two perpendicular axes lying in the plane. For a disc, if we consider two diameters, we can denote their moments of inertia as \( I_1 \) and \( I_2 \): \[ I = I_1 + I_2 \] Since the disc is symmetrical, \( I_1 = I_2 \). Therefore, we can write: \[ I = 2I_1 \] 3. **Relate the Moments of Inertia**: From the moment of inertia about the center (perpendicular to the plane), we have: \[ I = \frac{1}{2} m R^2 \] Thus, substituting into the equation from the perpendicular axis theorem: \[ \frac{1}{2} m R^2 = 2I_1 \] This simplifies to: \[ I_1 = \frac{1}{4} m R^2 \] 4. **Relate Moment of Inertia to Radius of Gyration**: The moment of inertia about the diameter can also be expressed in terms of the radius of gyration \( k \): \[ I_1 = m k^2 \] Setting the two expressions for \( I_1 \) equal gives: \[ m k^2 = \frac{1}{4} m R^2 \] 5. **Solve for the Radius of Gyration**: Dividing both sides by \( m \) (assuming \( m \neq 0 \)): \[ k^2 = \frac{1}{4} R^2 \] Taking the square root of both sides, we find: \[ k = \frac{R}{2} \] ### Final Result: The radius of gyration of a uniform circular disc of radius \( R \) about any diameter of the disc is: \[ k = \frac{R}{2} \] ---
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