If θ1 and θ2 be the apparent angles of dip observed in two vertical planes at right angles to each other, then the true angle of dip θ is given by
cot2θ = cot2θ1+ cot2θ2
tan2θ = tan2θ1+ tan2θ2
cot2θ = cot2θ1– cot2θ2
cot2θ = cot2θ1– cot2θ2
A.
cot2θ = cot2θ1+ cot2θ2
The ratio of resolving powers of an optical microscope for two wavelengths λ1 = 4000 Å and λ2 = 6000 Å is
8 : 27
9:4
3:2
3:2
Two Polaroids P1 and P2 are placed with their axis perpendicular to each other. Unpolarised light I0 is incident on P1. A third polaroid P3
is kept in between P1 and P2 such that its axis makes an angle 45o with that of P1. The intensity of transmitted light through P2 is
I0/2
I0/3
I0/8
I0/8
A beam of light from a source L is incident normally on a plane mirror fixed at a certain distance x from the source. The beam is reflected back as a spot on a scale placed just above the source L. When the mirror is rotated through a small angle θ, the spot of the light is found to move through a distance y on the scale. The angle θ is given by
y/2x
y/x
2y/x
2y/x
A thin prism having refracting angle 10° is made of glass of refractive index 1.42. This prism is combined with another thin prism of a glass of refractive index 1.7. This combination produces dispersion without deviation. The refracting angle of second prism should be
4°
6°
8°
8°