- A$\tan^{-1}\Big(\frac{3}{2}\Big)$
- B$\tan^{-1}\Big(\frac{2}{3}\Big)$
- C$\sin^{-1}\Big(\frac{2}{3}\Big)$
- D$\cos^{-1}\Big(\frac{3}{2}\Big)$
Explanation:
As $\vec{\text{A}}=2\hat{\text{i}}+2\hat{\text{j}},$ therefore Ax = 2 and Ay = 3. If $\theta$ is the angle which $\vec{\text{A}}$ encloses with y-axis, then.
$\tan\theta=\frac{\text{A}_\text{x}}{\text{A}_\text{y}}=\frac{2}{3}$ or $\theta=\tan^{-1}\Big(\frac{2}{3}\Big)$
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($A$) The center of mass of the assembly rotates about the $z$-axis with an angular speed of $\omega / 5$
($B$) The magnitude of angular momentum of center of mass of the assembly about the point $O$ is $81 m a^2 \omega$
($C$) The magnitude of angular momentum of the assembly about its center of mass is $17 \mathrm{ma}^2 \mathrm{\omega} / 2$
($D$) The magnitude of the $z$-component of $\vec{L}$ is $55 \mathrm{ma}^2 \omega$