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    Re: Basics of computing sunrise/sunset
    From: Frank Reed
    Date: 2009 Jun 22, 22:12 -0700

    I think we're largely talking at cross purposes here, and I may try to deal 
    with that further tomorrow, but for now I just want to talk about this 
    business of constant "surface brightness". I remember when I first learned 
    about it mathematically, in Astrophysics 201 or whatever it was called, over 
    25 years ago. And my first thought was, "huh? surface brightness can't be 
    changed by a telescope? Surely not." It's quite counter-intuitive, but the 
    physics is undeniable. As food for thought, here's a couple of quotes from 
    some astronomy and astrophysics textbooks that may be of interest for some of 
    you:
    
    [note: the correct astronomical/astrophysical term is "specific intensity" or just "intensity"]
    
    From Novotny's "Introduction to Stellar Atmospheres and Interiors":
    "No optical instrument can make a radiating surface appear more intense, since 
    it cannot increase the amount of energy passing along a ray. A telescope 
    gathers more light than the eye, but spreads it over an enlarged image. 
    Hence, the unresolved continuum of stars in the Andromeda Galaxy appears just 
    as disappointingly faint when viewed through a telescope as it does to the 
    naked eye."
    
    From Bradt's "Astronomy Methods":
    "Interesting implications of this equality B=I surround us, for example 
    starting a fire with a magnifying glass by focusing sunlight. Another 
    ramification is that radiation passing through an optical system has the same 
    brightness before and after its passage. Thus the moon has the same 
    brightness when viewed with bionuclars as when it is viewed with the naked 
    eyes. The image is bigger but the energy received per pixel of the retina, or 
    per square arcmin, is the same. This is true of the sun also. Thus the filter 
    material safe for naked eye viewing of the sun is also safe for viewing the 
    sun with binoculars as long as it fully covers both objective lenses."
    
    [the above should really mention that this refers to non-electronic optical 
    systems --those which do not add energy to the light-- so of course "night 
    vision" systems are not limited in this fashion]
    
    I looked around a bit hoping to find a nice web article on this topic, but 
    haven't had much luck. There's one from an NRAO astrophysics class here:
    http://www.cv.nrao.edu/course/astr534/Brightness.html
    which includes the following:
    "The conservation of brightness also applies to any lossless optical system, a 
    system of lenses and mirrors for example, that can change the direction of a 
    ray.  No passive optical system can increase the specific intensity or total 
    intensity of radiation.  If you look at the Moon through a large telescope, 
    the Moon will appear bigger (in angular size) but not brighter."
    
    -FER
    
    
    
    
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