For a particle performing linear $S.H.M.$ of amplitude '$r$',the potential energy is '$\lambda$' times its total energy. The displacement of the particle is

  • A
    $r\lambda$
  • B
    $\frac{r}{\lambda}$
  • C
    $r\sqrt{\lambda}$
  • D
    $\frac{r}{\sqrt{\lambda}}$

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