Two masses $A$ and $B$ of mass $M$ and $2M$ respectively are connected by a compressed ideal spring. The system is placed on a horizontal frictionless table and given a velocity $u \hat{k}$ in the $z$-direction as shown in the figure. The spring is then released. In the subsequent motion,the line from $B$ to $A$ always points along the $\hat{i}$ unit vector. At some instant of time,mass $B$ has an $x$-component of velocity as $V_x \hat{i}$. The velocity $\vec{V}_A$ of mass $A$ at that instant is:

  • A
    $V_x \hat{i} + u \hat{k}$
  • B
    $-V_x \hat{i} + u \hat{k}$
  • C
    $-2 V_x \hat{i} + u \hat{k}$
  • D
    $2 V_x \hat{i} + u \hat{k}$

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