(a) Note: The angles given are tricks. They are not measured from the normal, we must use the angle from normal.
Air → Plastic ni sin θi = nr sin θr, (1) sin (53) = nr sin(37) nr = 1.33
n = c /v 1.33 = 3x108 / v
v = 2.26 x 108 m/s
(b) Check the critical angle Plastic → Air. ni sin θc = nr sin (90) … (1.33) sin θc = (1) … θc = 48.75°

The incoming angle (53°) is larger than the critical angle, so total internal reflection will occur.
(c) This looks like a converging lens, but in lens problems, the lenses always have a higher index than the surrounding material. Since this ‘air lens’ has a smaller index of refraction it will behave the opposite as a normal lens would. From a simple refraction standpoint, there will be no refraction entering the air since the ray is perpendicular to the surface. Then on exiting, as you move less–more dense the ray bends towards the normal.
