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An inclined plane makes an angle of 60^(...

An inclined plane makes an angle of `60^(@)` with horizontal. A disc rolling down this inclined plane without slipping has a linear acceleration equal to

A

`(g)/(3)`

B

`(3)/(4)g`

C

`(g)/sqrt3`

D

`(g)/(2)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the linear acceleration of a disc rolling down an inclined plane at an angle of \(60^\circ\) with the horizontal, we can follow these steps: ### Step 1: Identify the formula for linear acceleration of a rolling body The linear acceleration \(a\) of a rolling body can be calculated using the formula: \[ a = \frac{g \sin \theta}{1 + \frac{k^2}{r^2}} \] where: - \(g\) is the acceleration due to gravity, - \(\theta\) is the angle of inclination, - \(k\) is the radius of gyration, - \(r\) is the radius of the disc. ### Step 2: Calculate the radius of gyration for a disc The radius of gyration \(k\) is given by: \[ k = \sqrt{\frac{I}{m}} \] For a disc, the moment of inertia \(I\) is: \[ I = \frac{1}{2} m r^2 \] Substituting this into the formula for \(k\): \[ k = \sqrt{\frac{\frac{1}{2} m r^2}{m}} = \sqrt{\frac{1}{2} r^2} = \frac{r}{\sqrt{2}} \] ### Step 3: Substitute \(k\) into the acceleration formula Now, substituting \(k = \frac{r}{\sqrt{2}}\) into the acceleration formula: \[ a = \frac{g \sin \theta}{1 + \frac{\left(\frac{r}{\sqrt{2}}\right)^2}{r^2}} = \frac{g \sin \theta}{1 + \frac{r^2/2}{r^2}} = \frac{g \sin \theta}{1 + \frac{1}{2}} = \frac{g \sin \theta}{\frac{3}{2}} = \frac{2g \sin \theta}{3} \] ### Step 4: Calculate \(\sin 60^\circ\) We know that: \[ \sin 60^\circ = \frac{\sqrt{3}}{2} \] ### Step 5: Substitute \(\sin 60^\circ\) into the acceleration formula Now substituting \(\sin 60^\circ\) into the equation for \(a\): \[ a = \frac{2g \cdot \frac{\sqrt{3}}{2}}{3} = \frac{g \sqrt{3}}{3} \] ### Step 6: Final result Thus, the linear acceleration of the disc rolling down the inclined plane is: \[ a = \frac{g \sqrt{3}}{3} \] ### Step 7: Simplify the expression This can also be expressed as: \[ a = \frac{g}{\sqrt{3}} \] ### Conclusion The final answer is: \[ \text{The linear acceleration of the disc is } \frac{g}{\sqrt{3}}. \] ---
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