$A$ 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. At a time $t < \frac{v_0 \sin \theta}{g}$,the angular momentum of the particle is

  • A
    $-mg v_0 t^2 \cos \theta \hat{j}$
  • B
    $mg v_0 t \cos \theta \hat{k}$
  • C
    $-\frac{1}{2} mg v_0 t^2 \cos \theta \hat{k}$
  • D
    $\frac{1}{2} mg v_0 t^2 \cos \theta \hat{i}$

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