Angular Momentum at Maximum Height
The magnitude of angular momentum \( L \) of a projectile at its maximum height (about the point of projection) is given by the cross product of its position vector \( \vec{r} \) and linear momentum \( \vec{p} \):
\[ L = \vec{r} \times \vec{p} \]
At the maximum height:
So, the position vector \( \vec{r} \) lies in the horizontal direction, and the velocity (hence momentum) is also horizontal. The angular momentum is mainly due to the vertical displacement and horizontal momentum:
\[ L = m v \cos \theta \cdot H = m v \cos \theta \cdot \frac{v^2 \sin^2 \theta}{2g} \]
Thus,
\[ L = \frac{m v^3 \cos \theta \sin^2 \theta}{2g} \]
This expression depends on \( \theta \), but interestingly, it turns out that for certain values of θ, the function has the same maximum value. However, for a full projectile motion, the angular momentum about the point of projection at maximum height remains constant because although height and horizontal momentum vary with angle, their product remains the same due to conservation laws.
Conclusion: The magnitude of angular momentum at the highest point remains constant with respect to the point of projection, regardless of the angle of projection \( \theta \).
The correct option is(D):
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: