According to Snell's Law, a wavefront of light (represented by a ray drawn in the direction perpendicular to the wavefront and in the direction of energy travel) will be bent as it moves from a media of one optical density into a media of differing optical density at any angle...

## See

This Answer NowStart your **48-hour free trial** to unlock this answer and thousands more. Enjoy eNotes ad-free and cancel anytime.

Already a member? Log in here.

According to Snell's Law, a wavefront of light (represented by a ray drawn in the direction perpendicular to the wavefront and in the direction of energy travel) will be bent as it moves from a media of one optical density into a media of differing optical density at any angle other than perpedicular to the surface. The relationship Snell developed is given by

N1Sin(theta1) = N2Sin(theta2)

Where N1 is the index of refraction for the media from which the ray originates, and theta1 is the angle it makes to the normal at the surface interface; N2 is the index of refraction for the media into which the ray travels, and theta2 is the angle the ray makes to the normal as it enters the new media.

For this example, the ray is originating at the fish in water which has an index of refraction of 1.33 and is striking the surface at some unknown angle theta1 to the normal. The ray leaves the water and enters air which has an index of refraction of 1.003 at an angle of 28.0 degrees to the normal.

Solving Snells equation for theta1 allows us to determine the unknown angle:

Sin(theta1) =(N2/N1)*sin(theta2)

invSin[Sin(theta1)] =invsin[(N2/N1)*sin(theta2)]

theta1 = invSin[(1.003/1.33)*sin(28.0)]

theta1 = invSin(0.3540) = 20.7deg.