$A$ dip needle lies initially in the magnetic meridian when it shows an angle of dip $\theta$ at a place. The dip circle is rotated through an angle $x$ in the horizontal plane and then it shows an angle of dip $\theta'$. Then $\frac{\tan \theta'}{\tan \theta}$ is

  • A
    $\frac{1}{\cos x}$
  • B
    $\frac{1}{\sin x}$
  • C
    $\frac{1}{\tan x}$
  • D
    $\cos x$

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