Two coherent sources separated by a distance $d$ are radiating in phase with a wavelength $\lambda$. $A$ detector moves in a large circle around the two sources in the plane of the two sources. The angular position of the $n = 4$ interference maxima is given as

  • A
    ${\sin ^{ - 1}}\frac{{n\lambda }}{d}$
  • B
    ${\cos ^{ - 1}}\frac{{4\lambda }}{d}$
  • C
    ${\tan ^{ - 1}}\frac{d}{{4\lambda }}$
  • D
    ${\cos ^{ - 1}}\frac{\lambda }{{4d}}$

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