Understanding the Focal Plan of Parallel Light Through a Thin Lens

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Discussion Overview

The discussion centers on the behavior of parallel light as it passes through a thin lens at an angle θ, specifically focusing on the mathematical proof of this phenomenon and the underlying principles involved.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants question why parallel light focuses on the focal plane when entering a thin lens at an angle θ and seek a mathematical proof for this behavior.
  • One participant suggests that the Thin Lens page on Wikipedia may provide helpful information regarding the topic.
  • Another participant emphasizes the need for proof that parallel light is not perpendicular to the lens.
  • A later reply introduces the concept of ray transfer matrices as a method to prove the focusing behavior of collimated beams, noting the specific matrix product used and its implications for the rays at the focal plane.

Areas of Agreement / Disagreement

The discussion reflects a lack of consensus, with participants expressing different needs for proof and varying approaches to understanding the focusing of parallel light through a thin lens.

Contextual Notes

Participants have not resolved the assumptions regarding the angle of incidence or the specific mathematical steps required to demonstrate the focusing behavior.

brianeyes88677
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Why does parallel light focus on the focal plan when enters a thin lens at an angle θ?
How to proof that mathematically?
 
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brianeyes88677 said:
Why does parallel light focus on the focal plan when enters a thin lens at an angle θ?
How to proof that mathematically?

Does the Thin Lens page at wikipedia help? http://en.wikipedia.org/wiki/Thin_lens

:smile:
 
I need the proof that the parallel light isn't perpendicular to the lens.
 
The proof can easily be done using the ray transfer matrices. In case you are not familiar with this term yet, navigate to this http://en.wikipedia.org/wiki/Ray_transfer_matrix_analysis
In describing focusing of a collimated beam (parallel rays) using such matrices, one uses the matrix product between thin lens matrix and free space propagation matrix in the order that the thin lens matrix is on the right. This order corresponds to the encounter of the ray bundle with the lens first, then propagate further behind it to reach the focal plane. The resulting matrix have the element A=0. This kind of ray transfer matrix is termed as having focusing behavior, and you will see at the end of your calculation that the heights of all rays at the focal plane are equal, which physically means they are being focused.
 

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