Given:
We are to calculate: Angular momentum \( \vec{L} \) and torque \( \vec{\tau} \) w.r.t. origin, especially at the point \( (\ell, -h) = (10, -1) \)
At t = 0:
At the point (x = +10, y = -1):
This is a displacement of 20 m along x-axis from the starting point, so using:
\[ x = ut + \frac{1}{2}at^2 \Rightarrow 20 = 0 + \frac{1}{2} \cdot 10 \cdot t^2 \Rightarrow t^2 = 4 \Rightarrow t = 2\,\text{s} \]
Velocity at this point: \( v = at = 10 \cdot 2 = 20\, \text{m/s} \)
Position vector: \( \vec{r} = 10\hat{i} - 1\hat{j} \)
Linear momentum: \( \vec{p} = M\vec{v} = 0.2 \cdot 20\hat{i} = 4\hat{i} \)
Angular momentum:
\[ \vec{L} = \vec{r} \times \vec{p} = (10\hat{i} - \hat{j}) \times (4\hat{i}) = -\hat{j} \times 4\hat{i} = 4\hat{k} \]
β Correct: Option C β Angular momentum is \( \vec{L} = 4\hat{k} \) at \( (10, -1) \)
Correct Answer: Option C
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 mΒ².
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
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: