$A$ small particle of mass $m$ is projected at an angle $\theta$ with the $x$-axis with an initial velocity $v_{0}$ in the $x-y$ plane as shown in the figure. For time $t < \frac{v_{0} \sin \theta}{g}$,the angular momentum of the particle is (where $\hat{i}, \hat{j}$ and $\hat{k}$ are unit vectors along the $x, y$ and $z$ axes respectively):

  • A
    $-\frac{1}{2} mg v_{0} t^{2} \cos \theta \hat{k}$
  • B
    $-mg v_{0} t^{2} \cos \theta \hat{k}$
  • C
    $mg v_{0} t \cos \theta \hat{k}$
  • D
    $\frac{1}{2} mg v_{0} t^{2} \cos \theta \hat{k}$

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