Parallel light rays refraction by glass hemisphere problem

Click For Summary
SUMMARY

The discussion focuses on the refraction of parallel light rays through a glass hemisphere with radius R and an index of refraction ng greater than that of air. The participant utilized the paraxial approximation and the lens maker's equation, adjusting for the concave nature of the surface, to derive the image distance s' as R(n2/(n1-n2)). Additionally, the effect of a 0.5% increase in the index of refraction on the focus point was analyzed, concluding that the new index can be calculated by multiplying n2 by 1.005.

PREREQUISITES
  • Understanding of paraxial ray approximation
  • Familiarity with the lens maker's equation
  • Knowledge of refraction indices
  • Basic principles of optics and light behavior
NEXT STEPS
  • Study the derivation of the lens maker's equation in detail
  • Explore the implications of the sign convention for refracting surfaces
  • Investigate the effects of varying indices of refraction on light paths
  • Learn about advanced optical systems involving multiple lenses
USEFUL FOR

Students and professionals in optics, physics educators, and anyone involved in optical design or studying light behavior in different media.

marational
Messages
4
Reaction score
0

Homework Statement


Parallel light rays travel from air towards a glass hemisphere with radius R and
index of refraction ng > nair. A top view is shown in the figure.
http://img8.imageshack.us/img8/6380/parallellightrays.jpg
(a) Determine where the light rays come to a focus relative to the point P.
(b) The index of refraction of the hemisphere is increased by 0.5 percent. Does the
focus point change from that in part (a)? If it changes, then by how much?

Homework Equations


I found an equation in the textbook for paraxial rays approaching a spherical surface that is convex towards them. In that situation, the second medium was some glass, and the original medium was air. The equation was given as follows:
n1/s + n2/s' = (n2-n1)/R
where s is object distance (from which the paraxial rays originated) from the surface, and s' is the distance of the image formed from the surface. R is the radius of the sphere.

The Attempt at a Solution


The big difference between the two scenarios is that in the actual problem, the rays are approaching a surface that is concave towards them, rather than convex. However, the textbook states that according to the sign convention for refracting surfaces, R is positive when convex toward the object, and negative when concave toward the object.
I simply put this into the equation to give
n1/s + n2/s' = (n2-n1)/-R
n1/s + n2/s' = (n1-n2)/R
where n1 is the index of refraction for the glass, and n2 is the index for air
The other issue was that there isn't really an object distance in the problem.
Since the rays are parallel, I set s to infinity (making n1/s = 0) and arranged for s'.
n2/s' = (n1-n2)/R
R(n2/(n1-n2)) = s'

I suppose this would be my final answer for part a, but I'm unsure if my method works.

If I'm correct, I figured that for part b I could simply multiply n2 by 1.005.

Any help would be appreciated.
 
Last edited by a moderator:
Physics news on Phys.org
It looks correct.

ehild
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 15 ·
Replies
15
Views
2K
Replies
11
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K