The horizontal acceleration that should be given to a smooth inclined plane of angle $\theta = \sin^{-1}\left(\frac{1}{l}\right)$ to keep an object stationary on the plane, relative to the inclined plane is:

  • A
    $\frac{g}{\sqrt{l^2-1}}$
  • B
    $g \sqrt{l^2-1}$
  • C
    $\frac{\sqrt{l^2-1}}{g}$
  • D
    $-\frac{g}{\sqrt{l^2+1}}$

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