A circular ring and a solid sphere having same radius roll down on an inclined plane from rest without slipping. The ratio of their velocities when reached at the bottom of the plane is $\sqrt{\frac{\mathrm{x}}{5}}$ where $\mathrm{x}=$ _______.
We are given a circular ring and a solid sphere, both having the same radius \( R \), rolling down an inclined plane from rest without slipping. We need to find the ratio of their linear velocities at the bottom of the incline, expressed as:
\[ \frac{v_{\text{ring}}}{v_{\text{sphere}}} = \sqrt{\frac{x}{5}} \] and determine the value of \( x \).
When a rigid body rolls down an incline without slipping, the loss of potential energy is converted into both translational and rotational kinetic energies:
\[ mgh = \frac{1}{2} m v^2 + \frac{1}{2} I \omega^2 \]
Using the rolling condition \( v = R\omega \), we can rewrite the equation as:
\[ mgh = \frac{1}{2} m v^2 \left(1 + \frac{I}{mR^2}\right) \]
Thus, the velocity of the object at the bottom is given by:
\[ v = \sqrt{\frac{2gh}{1 + \frac{I}{mR^2}}} \]
Step 1: For the circular ring:
\[ I_{\text{ring}} = mR^2 \] \[ v_{\text{ring}} = \sqrt{\frac{2gh}{1 + \frac{I_{\text{ring}}}{mR^2}}} = \sqrt{\frac{2gh}{1 + 1}} = \sqrt{\frac{2gh}{2}} = \sqrt{gh} \]
Step 2: For the solid sphere:
\[ I_{\text{sphere}} = \frac{2}{5}mR^2 \] \[ v_{\text{sphere}} = \sqrt{\frac{2gh}{1 + \frac{2}{5}}} = \sqrt{\frac{2gh}{\frac{7}{5}}} = \sqrt{\frac{10gh}{7}} \]
Step 3: Find the ratio of their velocities.
\[ \frac{v_{\text{ring}}}{v_{\text{sphere}}} = \frac{\sqrt{gh}}{\sqrt{\frac{10gh}{7}}} = \sqrt{\frac{7}{10}} \]
Step 4: Compare with the given form.
\[ \sqrt{\frac{7}{10}} = \sqrt{\frac{x}{5}} \]
Step 5: Equate the two expressions inside the square roots:
\[ \frac{7}{10} = \frac{x}{5} \]
Step 6: Solve for \( x \).
\[ x = \frac{7}{10} \times 5 = 3.5 \]
Therefore, the value of \( x \) is:
\[ \boxed{x = 3.5} \]
Final Answer: \( x = 3.5 \)
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