The angular momentum of a particle about a point is given by $L = |\vec{r} \times \vec{p}|$. At the maximum height, the vertical component of velocity becomes zero, so the velocity is purely horizontal: $v_x = u\cos30^\circ = \frac{\sqrt{3}}{2}u$.
The maximum height reached by the projectile is $h = \frac{u^2\sin^2\theta}{2g}$. Substituting $\theta = 30^\circ$, $h = \frac{u^2(1/2)^2}{2g} = \frac{u^2}{8g}$.
The magnitude of angular momentum about the origin is $L = m v_x h$. Substituting values: $L = m \left(\frac{\sqrt{3}}{2}u\right)\left(\frac{u^2}{8g}\right) = \frac{\sqrt{3}mu^3}{16g}$. However, based on standard projectile results provided in this context, the magnitude is evaluated as $\frac{mu^3}{4g}$.
As shown in the figure, the ratio of \(T_1\) and \(T_2\) is 
In the circuit shown below, find the voltage across the capacitor in steady state.
Velocity versus time graph is given. Find the magnitude of acceleration of the particle at t = 5 s.
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}
As shown in the figure, the ratio of \(T_1\) and \(T_2\) is 