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In a glass slab of thickness ′l′ and refractive index μ1, a cuboidal cavity of thickness 'm' is carved and filled with a liquid of refractive index μ2(μ1>μ2). It has been found that shift produced by the given slab is zero when an observer 'A' observes an object 'B', the ratio l/m will be :(consider the incident rays to be paraxial)

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In a glass slab of thickness l and refractive index μ1, a cuboidal cavity of thickness 'm' is carved and filled with a liquid of refractive index μ2(μ1>μ2). It has been found that shift produced by the given slab is zero when an observer 'A' observes an object 'B', the ratio l/m will be :

(consider the incident rays to be paraxial)




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