alexis wrote:I see you remain unconvinced. Well, the claim is easy to put to test: take your favourite telescope, point it in a random direction in the night sky with a low power eye-piece (say 50x). Count the stars. Do the same with a high power eye-piece (say 300x). Are the number of stars the same? I think you will find they are not. The reason is simple: the telescopic image of a star is not a point but a finite size point spread function (PSF) that also scales with the magnification, so the contrast remains constant. In addition, think of the implications if one could observe arbitrary faint stars by just increasing the image scale!
/Alexis
Well, while the following arguments are certainly not
necessary in order to justify my AutoMag scheme, it may be just
interesting to discuss this issue in some greater depth;-):
An excellent and standard reference on these matters is the book
"Visual Astronomy of the Deep Sky", written by the physicist Roger.N. Clark, Ph.D.
Since you do not seem to believe me (well, I usually work on construction sites;-)),
let me quote from page 49 of that book. The chapter is called
"The Faintest star Visible in a Telescope".
"The eye's fundamental limit is around 50 to 150 photons of green light
arriving over a several second period, corresponding to a star as faint
as 8.5m." (t00fri:) Normally, depending on the observer's location,
one may only see stars of 5m - 7m with the naked eye. "Magnification does not
change the brightness of a point source in the telescope, but it does decrease
the surface brightness of the background (in agreement with my previous statement above)
and reduces the field of view so other stars do not interfere. Therefore, the
fundamental limits of the eye can be reached when a telescope is used. Here it really
is possible to see the equivalent of 8.5m stars naked-eye" (clearly your above
extrapolation to infinitely faint star detection is nonsensical)!
"A star image is actually a diffraction disk, but it is so small that, if faint,
the disk is a point to the eye at any reasonable magnification at all"
(t00fri: this of course invalidates your PSF argument above...
we construction workers call this the "correspondence principle", connecting smoothly
between the laws governing the wave regime of light and geometrical optics)
"The fundamental magnitude limit M_t of a telescope is given by
M_t = M_e + 2.5 log_10 (D^2 t/D_e^2),
where M_e is the eye limiting magnitude (8.5 at best), D=telescope diameter,
D_e is the eye diameter (7.5mm), and t=telescope transmission factor ~0.7.
The surface brightness M_b of the sky or an extended object is darkened by the
/telescope magnification m/ and transmission factor t as follows
M_b = -2.5 log_10 (D^2 t/m^2 D_e^2)
This is why the magnification helps to detect faint stars when the sky is bright,
or even under dark country skies compared to when /low power is used/!"
And then in that book you may inspect detailed diagrams about actual
measurements of the effect of telescope magnification
on the faintest visible stars etc...
Bye Fridger