A rod of length \(l\) resting on a wall and the floor. Its lower end \(A\) is pulled towards right with a…
- \(\frac{v}{l \cos \theta}\)
- \(l \cos \theta\)
- \(\frac{v}{l \sin \theta}\)
- \(\frac{v}{{l}^{2} \cos \theta}\)
Solution
It means the velocities of ends of rod along its length must be equal.
$\begin{aligned} v_{A} \sin \theta &= v_{B} \cos \theta \Rightarrow v_{B} = v_{A} \frac{\sin \theta}{\cos \theta} = v \tan \theta \\ \text{or } \quad v_{B} &= v \tan \theta \quad \text{...(i)} \end{aligned}$ Then, $\omega_{B A} = \frac{v_{B A_{\perp}}}{l} = \frac{\left|v_{A} \cos \theta - \left(-v_{B} \sin \theta\right)\right|}{l}$ \(\Rightarrow \quad \omega_{B A}=\frac{v_{A} \cos \theta+v_{B} \sin \theta}{l}\) ...(ii)
Using Eqs. (i) and (ii),
\(\omega_{B A}=\frac{v}{l \cos \theta}\)
This is also angular velocity of rigid body about its centre of mass.
.Asked in: JEE Mains - Motion In One Dimension - Test 4