A beam of diameter d is incident on a glass hemisphere as shown in figure. If the radius of curvature of the hemisphere is very large in comparison to d, then diameter of the beam at the base of the hemisphere will be
3d4
Refraction at the curved surface μ2v−μ1u=μ2−μ1R
PP1 is very small
P1P1D=BCCDAP1=d,P1D=v