In a thick glass slab of thickness l, and refractive index n1 a cuboidal cavity of thickness 'm' is carved as shown in figure and is filled with a liquid of RI n2 (n1 > n2). The ratio l/m, so that shift produced by this slab is zero when an observer r4 observesan object B with paraxial rays is
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In a thick glass slab of thickness l, and refractive index n1 a cuboidal cavity of thickness 'm' is carved as shown in figure and is filled with a liquid of RI n2 (n1 > n2). The ratio l/m, so that shift produced by this slab is zero when an observer r4 observesan object B with paraxial rays is