An object starts from rest and is acted upon by a variable force $F$ as shown in the figure. If $-F_0$ is the initial value of the force at $x=0$,then the position of the object where it again comes to rest will be:

  • A
    $\frac{2 F_0}{\tan \alpha}$
  • B
    $\frac{F_0}{\sin \alpha}$
  • C
    $\frac{2 F_0}{\cot \alpha}$
  • D
    $\frac{F_0}{2 \cos \alpha}$

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