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A converging lens forms a real image I of an object on its principle axis. A rectanglular slab of refractive index and thickness x is introduced between I and the lens. Image I will move

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towards the lens by $(μ - 1) x$

away from the lens by $(1 - \frac{1}{μ}) x$

away from the lens by $(μ - 1) x$

towards the lens by $(1 - \frac{1}{μ}) x$

answer is B.

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$shift = x [1 - \frac{1}{μ}] Away from lens$

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