Step 1: Formula for Acceleration in Rolling Motion:
- For a cylinder rolling down an incline, the acceleration \( a \) is given by:
\[ a = \frac{g \sin \theta}{1 + \frac{I_{cm}}{MR^2}} \]
- For a solid cylinder, \( I_{cm} = \frac{1}{2} MR^2 \).
Step 2: Substitute Values:
\[ a = \frac{g \sin \theta}{1 + \frac{1}{2}} \]
- Given \( g = 10 \, \text{m/s}^2 \) and \( \theta = 60^\circ \) (so \( \sin 60^\circ = \frac{\sqrt{3}}{2} \)):
\[ a = \frac{10 \times \frac{\sqrt{3}}{2}}{1 + \frac{1}{2}} \]
Step 3: Calculate \( a \):
\[ a = \frac{10 \times \frac{\sqrt{3}}{2}}{\frac{3}{2}} = \frac{10 \sqrt{3}}{3} = \frac{x}{\sqrt{3}} \]
- Therefore, \( x = 10 \).
So, the correct answer is: \( x = 10 \)
Step 1: Formula for acceleration of a rolling object on an incline.
For a body rolling without slipping on an inclined plane of angle \( \theta \): \[ a = \frac{g \sin \theta}{1 + \frac{k^2}{R^2}} \] where \( k \) is the radius of gyration and \( R \) is the radius of the body.
Moment of inertia for a solid cylinder: \[ I = \frac{1}{2} mR^2 \Rightarrow \frac{k^2}{R^2} = \frac{1}{2} \] Substitute in the formula: \[ a = \frac{g \sin \theta}{1 + \frac{1}{2}} = \frac{g \sin \theta}{\frac{3}{2}} = \frac{2g \sin \theta}{3} \]
\[ \theta = 60^\circ, \quad g = 10\,\text{m/s}^2 \] \[ a = \frac{2 \times 10 \times \sin 60^\circ}{3} \] \[ a = \frac{20 \times \frac{\sqrt{3}}{2}}{3} = \frac{10\sqrt{3}}{3}\,\text{m/s}^2 \]
Acceleration = \( \frac{x}{3} \, \text{m/s}^2 \) \[ \frac{x}{3} = \frac{10\sqrt{3}}{3} \Rightarrow x = 10\sqrt{3} \] \[ \text{Hence, } x = 10 \]
\[ \boxed{x = 10} \]
If $\overrightarrow{\mathrm{L}}$ and $\overrightarrow{\mathrm{P}}$ represent the angular momentum and linear momentum respectively of a particle of mass ' $m$ ' having position vector $\overrightarrow{\mathrm{r}}=\mathrm{a}(\hat{\mathrm{i}} \cos \omega \mathrm{t}+\hat{\mathrm{j}} \sin \omega \mathrm{t})$. The direction of force is
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.
Which of the following are correct expression for torque acting on a body?
A. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{L}}$
B. $\ddot{\tau}=\frac{\mathrm{d}}{\mathrm{dt}}(\ddot{\mathrm{r}} \times \ddot{\mathrm{p}})$
C. $\ddot{\tau}=\ddot{\mathrm{r}} \times \frac{\mathrm{d} \dot{\mathrm{p}}}{\mathrm{dt}}$
D. $\ddot{\tau}=\mathrm{I} \dot{\alpha}$
E. $\ddot{\tau}=\ddot{\mathrm{r}} \times \ddot{\mathrm{F}}$
( $\ddot{r}=$ position vector; $\dot{\mathrm{p}}=$ linear momentum; $\ddot{\mathrm{L}}=$ angular momentum; $\ddot{\alpha}=$ angular acceleration; $\mathrm{I}=$ moment of inertia; $\ddot{\mathrm{F}}=$ force; $\mathrm{t}=$ time $)$
Choose the correct answer from the options given below:
A wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg m².
A tube of length 1m is filled completely with an ideal liquid of mass 2M, and closed at both ends. The tube is rotated uniformly in horizontal plane about one of its ends. If the force exerted by the liquid at the other end is \( F \) and the angular velocity of the tube is \( \omega \), then the value of \( \alpha \) is ______ in SI units.
