Here’s a sidebar from my graphics texxtbook on shortest path:

Sidebar 6.1 Finding the Angle of Reflection
Our derivation of the angle of reflection began with the principle that the 
angle of reflection equals the angle
of incidence. This principle was known to Euclid and Ptolemy 2000 years ago. 
Hero of Alexandria showed that
this path was the shortest from the source to the eye (see Exercise 6.13). If 
wasn’t until the early 17th century
that Fermat stated a more general version known as the principle of least time. 
However, none of these works
was based on the physics of light propagation but rather on the observation 
that light took the shortest (fastest)
path. Hence they did not explain why the angle of reflection equaled the angle 
of incidence nor why light didn’t
take multiple paths. It wasn’t until later in the 17th century that Huygens 
used the wave nature of light to
derive the angle of reflection.

From the above, refraction follows as does the lifeguard problem.

Ed


__________

Ed Angel

Founding Director, Art, Research, Technology and Science Laboratory (ARTS Lab)
Professor Emeritus of Computer Science, University of New Mexico

1017 Sierra Pinon
Santa Fe, NM 87501
505-984-0136 (home)                     edward.an...@gmail.com
505-453-4944 (cell)                             http://www.cs.unm.edu/~angel

> On Feb 16, 2020, at 10:33 PM, _ Bruno W <wbr...@gmail.com> wrote:
> 
> Not sure about the natural selection, but here are 2 small (possibly 
> important) corrections.
> 1.  The lifeguard is still to the left of the swimmer when the lifeguard hits 
> the water.  But by a much smaller distance than if
> he had ran straight at the swimmer.
> 2.  The most widely accepted explanation for the origin of the least action 
> principle has to do with waves or paths, and doesn't
> require the photon to know in advance where it should go.
> In one version, the wave function of the photon goes out in all directions 
> with a phase at any point given by exp(iS/hbar) where
> S is the action.  Because hbar is small, the waves oscillate rapidly and 
> generally cancel out everywhere, except of course
> when the derivative of the action is zero and the wave stops oscillating 
> completely.  This will happen at the path of least (or in some
> cases greatest) action.
> Feynman did this one better by saying you don't need waves, you integrate 
> over all paths, and you get to include all kinds
> of crazy paths, even ones that go in crazy loops and backwards in time and 
> whatever.  Once again the extreme action paths
> are the only ones that survive in the classical limit (hbar -> 0).
> Hope this helps?
> 
> On Sun, Feb 16, 2020 at 10:05 PM <thompnicks...@gmail.com 
> <mailto:thompnicks...@gmail.com>> wrote:
> Hi, Everybody, and Steve, and Miles
> 
>  
> 
> Please everybody forgive me for what I am about to garble.
> 
>  
> 
> Steve Guerin and I have a long standing argument concerning the above 
> question.  He thinks my answer to the above question will be “natural 
> selection.”  His answer to that question is, is that as energy flows from 
> high to low concentrations, it seeks, and finds the most efficient route. 
> Today, steve presented to me a most astounding example, which I am sure most 
> of you are familiar with, but which I had never quite grasped.  It is 
> illuminated by a metaphor.  Imagine a beach and a lifeguard standing on the 
> beach when a drowning swimmer calls out to the lifeguard’s right.  Should the 
> lifeguard run directly toward the drowning swimmer.  No, because he can make 
> a lot faster progress toward the swimmer while running on the beach than he 
> can while swimming.  So he should chose a path that minimizes his time to the 
> swimmer, not the path directly toward the swimmer.  That path, the path of 
> least action, will carry him to the right of the swimmer until he reaches he 
> water’s edge and starts to swim.   Lifeguards have to be trained to do this, 
> and lifeguards argue about which direction to head off under  under which 
> conditions. 
> 
>  
> 
> Well, light approaching boundary between air and water faces the same 
> situation.  And the stunning fact is that light finds the least action path.  
> As I understand it, the light leaves the source in a direction that takes 
> into account the boundary that it is approaching.  PLEASE correct me if I 
> have this wrong. Yet, of course, in this situation there is no trial and 
> error.  Photons of light just “know” how to do this.  If this is true, I 
> promise NEVER to yawn again when one of you is going on about quantum 
> physics. 
> 
>  
> 
> Now, Steve, èIFç I understood you, you also went on to describe ants behavior 
> and lightening behavior as analogous processes that also find Least Action 
> Pathways.  And, I think you are also going to perhaps assert that a tornado 
> is a structure that facilitates a least action pathway. Etc.  But these are 
> plainly “historical” processes. I.e, in all cases the process tries out 
> options, and settles on  the LAP.  But with light, here is no history.  
> Photons are like lifeguards who know instinctively what path to set out on to 
> reach the swimmer with the least action
> 
>  
> 
> Could I possibly have this right?  Once we get this first bit straightened 
> out, I have a question about its relation to natural selection.
> 
>  
> 
> Nick
> 
>  
> 
> Nicholas Thompson
> 
> Emeritus Professor of Ethology and Psychology
> 
> Clark University
> 
> thompnicks...@gmail.com <mailto:thompnicks...@gmail.com>
> https://wordpress.clarku.edu/nthompson/ 
> <https://wordpress.clarku.edu/nthompson/>
>  
> 
>  
> 
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