A beam of light AO is incident a glass slab `(mu=1.54)` in the direction show. The reflected ray OB is passed through a Nicol prism. On viewing through a Nicol prism, we find on rotating the prism that

A beam of light AO is incident on a glass slab (mu=1.54) in a direction as shown in figure. The reflected ray OB is passed throught a Nicol prism. On viewinf through a Nicole prism, we find rotating the prism that (tan^(-1)1.54=57^(@))

A beam of light AO is incident on a glass slab (mu=1.54) in a direction as shown in figure. The reflected ray OB is passed throught a Nicol prism. On viewinf through a Nicole prism, we find rotating the prism that (tan^(-1)1.54=57^(@))

A beam of light AO is incident on a glass slab ( mu=1.54 ) in a direction as shown in the diagram The reflected ray OB is passed through a polaroid On viewing through the polaroid. We find that on rotating the polaroid (given tan 57^@=1.54 )

A light beam is incident on a rectangular glass plate (mu= 1.54) The reflected light OB passes through a nicol prism. On observing the transmitted light while rotating the prism, it is seen that

A beam of light is incident on a glass slab (mu = 1.54) in a direction as shown in the figure. The reflected light is analysed by a polaroid prism. On rotating the polaroid, (tan 57^(@) = 1.54)

A beam of light is incident on a glass slab (mu = 1.54) in a direction as shown in the figure. The reflected light is analysed by a polaroid prism. On rotating the polaroid, (tan 57^(@) = 1.54) (##DPP_PHY_CP24_E01_002_Q01.png" width="80%">

A beam of light is incident on a glass slab (mu = 1.54) in a direction as shown in the figure. The reflected light is analysed by a polaroid prism. On rotating the polaroid, (tan 57^(@) = 1.54) (##DPP_PHY_CP24_E01_002_Q01.png" width="80%">