A beam of light is converging towards a point on the screen. If a plane parallel plate of glass of refraactive in μ and thickness t is introduced in the path of the beam, the convergent point is shifted
When glass plate of thickness t is introduced, the optical path increases by (t/μ).
So the convergence point shifts by t – (t/ μ)
i.e. t[1 – (1/ μ)] nearer.