To determine the height by which the outer rail should be raised, we use the concept of railway banking, which involves balancing the centripetal force needed to negotiate a curve with the gravitational force on the inclined plane. The formula for the height \(h\) of the outer rail is given by:
\(h = \frac{v^2b}{gR}\)
where:
Plugging these values into the formula, we have:
\(h = \frac{(12)^2 \cdot 1.5}{10 \cdot 400}\)
Simplifying:
\(h = \frac{144 \cdot 1.5}{4000}\)
\(h = \frac{216}{4000}\)
\(h = 0.054 \, \text{m}\)
Converting this into centimeters, we find:
\(h = 5.4 \, \text{cm}\)
Thus, the height by which the outer rail should be raised is 5.4 cm.
Therefore, the correct answer is 5.4 cm.
For a train moving around a curve, the required banking angle θ is given by:
\[\tan \theta = \frac{v^2}{Rg}\]
where \(v = 12 \, \text{m/s}\), \(R = 400 \, \text{m}\), and \(g = 10 \, \text{m/s}^2\).
Substitute the values:
\[\tan \theta = \frac{12^2}{10 \times 400} = \frac{144}{4000} = \frac{h}{1.5}\]
where \(h\) is the height by which the outer rail should be raised over the inner rail, and the distance between the rails is 1.5 m.
Solving for \(h\):
\[h = \frac{144 \times 1.5}{4000} = 5.4 \, \text{cm}\]
Thus, the required height is 5.4 cm.
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.
