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Re: [APML] 7331 (again!)
>From: Joe Pedit <pedit@email.unc.edu>
>Reply-To: astro-photo@seds.org
>To: astro-photo@seds.org
>Subject: Re: [APML] 7331 (again!)
>Date: Sat, 22 Sep 2001 08:31:27 -0400
>
>Joseph Dartsum wrote:
> >
> > Can you describe your definition of signal to noise ratio, and what
> > operations in Picture Window contribute to increasing it?
> >
>
>Joe D.,
>I would be interested in hearing how you would define signal and noise
>in scanned film images? What methods would you use to increase the
>signal to noise ratio in scanned film images? Would you use methods
>that would alter the spatial aspect of noise (i.e., alter the range of
>the semivariogram)?
>Joe P.
It's pretty obvious..
Let's consider CCD, where each pixel has a linear response with Poisson
counting statistics. It's sqrt(S), where S=signal counts. The greater the
signal, the greater the S/N ratio.
Let's consider film, where we consider a "point" (mathematically speaking).
It's a well known phenomenon, that you can go 1 to 2 stops overexposure and
get a decent printable negative AND you get better (finer) grain. (due to
the non-uniform distribution of film grains) This is the same situation as
above: more exposure gives you less grain (throughout the entire negative),
i.e. less noise characterstics in shadow..nominal.. highlight areas. Film
has the unfortunate additional problem of "scattering", which adds a
Gaussian type blur to its response, which complicates the signal to noise
issue even further. (Take shot of an object using TP2415 and color
film..the TP will show guiding/seeing errors, the color film will show nice,
round stars. The latter is film-grain based Guassian blur, which often
misleads amateurs into thinking they are getting beautifully guided, high
resolution images. NOT!).
The answer to your question is very simple, use a single long exposure
negative, well guided, under optimal seeing conditions. It's the same
conclusion in Dr. Mike Newberry's CCD article (see CCD Astronomy article),
where he went thru some long and detailed algebraic calculations. Like he
says, "it's nothing more than we already knew". The catch, is that long
exposures "trap" you for averaging effect of seeing, which is a killer: this
will destory high-resolution imagery. So, you inevitably run into a
paradox, or what you would know as an engineering tradeoff. Short exposures
to "freeze" seeing (fractions of seconds), or long exposures to increase S/N
ratio.
Fundamental result: S/N ratio increases according to S, the bigger S is the
better.
The amateur community is misquoting a "result" on combination of images to
improve S/N ratio, which indicates there non-understanding of BASIC
probability theory. I'm sure you are aware of this. S/N ratio implies the
*knowledge* of a probability-density function, i.e. the signal has been
infinitely sampled to determine this (which is impossible), from which you
can calculate the mean/std-dev = S/N ratio. From 2 to 3 (or whatever number
of film images you've taken), this is obviously way UNDER sampled..you have
no idea about the measurement statistics, with so few samples. Amateurs are
using another definition of "signal to noise" ratio (not the strict
definition, as used by scientists and mathematicians), which is simply their
false non-scientific impression..pseudo-science. It's been widely quoted in
print, web articles by amateurs.
When Tony Hallas states the following:
Hello everyone,
Last night I used TWO HOUR hypered Kodak Royal Gold 200 @ 90 minute
exposures of 7331 (great test object) and recorded a LOT more than the
previous
negatives. Tracking was very good, as was the focus this time. I "polluted"
these better negatives with the original Picture Window result and came up
with
a new image and a close up.. you can see H II regions and galaxies
everywhere...
in the close up, the companion galaxy to the upper left even has two faint H
II
regions showing. As the signal to noise ratio is increased through PW more
detail and color is showing up... almost CCD! :-)
*******************************************
Look at what he says. He's got 2 new negatives (better S/N ratio) combined
with a previous result (poorer S/N ratio). This makes no sense. Of course,
the resultant image will be no better (in terms of S/N ratio), than the
poorer image. (See Dr. Mike Newberry's 3 part article in CCD Astronomy, on
signal to noise ratio, it's a simple algebraic calculation at a junior high
school level). You don't even have to do math to understand this, anyone
knows: "the system response is no stronger than the weakest link". The
"weak link", is the negative with the poorer S/N ratio. You NEVER want to
combine images with varying S/N ratio, period. This is widely done in the
amateur community, which is laughable.
If you look at his use of the word "polluted" (destroying high resolution),
you can tell even he can tell that the resultant image is poorer than what
he started out with. The whole evaluation process of astrophotography is so
SUBJECTIVE (judging images by human eye & how "aesthetic" they are), any
critical analysis is by definition..undefined. Tony Hallas never bothered
to answer my question about signal to noise ratio, so that's very telling..
His Sky & Telescope article has some glaring errors in this respect. It's
also a poor reflection on S&T editorial, which claims to be the "Essential
Resource in Astronomy". Not.
Amateurs should stay within their domain, "pretty pictures". Do NOT go into
an area, where you do not have any expertise, like mathematical statements
on signal to noise ratio (or any science). You guys are leaving a
paper-trail, which will come back to haunt you. It's a simple matter of
quoting these posts, web-sites...instant loss of credibility. At the last
AAS (American Astronomical Society) meeting, the word from professionl
astronomers was that collaboration between amateurs and professionals
was...DEAD. The automated tracking systems (meteors, comet trackers/LINEAR,
supernova) have completely eliminated the existing form of amateur
contributions. The foulup of "signal to noise ratio", as given by the
above, is further evidence that amateurs have nothing meaningful (in a
technical sense) to contribute. If these statements were presented in a
technical forum (ASP, Astronomical Society of the Pacific, meeting), they
would LAUGH AT YOU. (the above was some simple junior high school level
algebraic calculations. Or, just basic systems-level concepts
understandable by the avg layman). There were stories floating around about
ludicrous statements made by amateurs, which drawing a great deal of
ridicule and laughter. I'm afraid the Internet has highlighted the problem
with amateurs, and put the nail-in-the-coffin, for any cooperative pro-am
work. Amateurs have become irrelevant. Not only that, they are
incriminating themselves for being a bunch of pseudo-scientists, like
Face-On-Mars crackpots.
The "pretty picture" that was posted by Tony Hallas is just THAT. A "pretty
picture". This is a nice way of saying, it has no technical merit. (all
the rave comments about h-alpha regions, small galaxies, are simply
gibberish). Try taking the same picture with a 14" Cass from space (without
the corruptive effects of seeing, destroying high resolution). The
resultant image will blow away the land-based one easily. The only effect I
see from Tony's hypering (which was totally hit-and-miss, no quantitative
way of graphing out the effects of hypering), was compensating for the
Schwarzchild exposure (threshold effect) of film. You will record fainter
stuff. His claims of better signal to noise, is simply gibberish.
FILM:
1. threshold effect
2. "Gaussian Blur" induced by grain scattering
3. non-linear response, "S" shaped curve
4. other effects
The only thing I saw from the posted images, was attritutable to 1. The
effects of 2) will always be there, & CCD will always have the edge there.
"the worst part of the telescope is the atmosphere"
..as quoted by Thierry Legault (one of the group of French high-resolution
astro imagers)
Look at the cumulative effect of seeing, of several hrs of exposure (3
negatives)..this plus the "Gaussian Blur" effect of film-grain scattering,
destroys any concept of "high-resolution" in Tony's images. (just admiring
the "pretty picture" is deceptive..it's not as good, as what COULD be
obtained. Look at Legault's Saturn & Jupiter pics, where he took image upon
image, throwing away the corrupted images due to "seeing". They look like
space-borne telescope images).
Tony Hallas wrote:
< 2 second STV exposures>
< .5 sec exposures!! approaching 1/3 arc-sec resolution>
Dude, don't make me laugh, ok? 2 second exposures?? You're AVERAGING the
cumulative effects of seeing.. While your STV is merrily _sitting there_
exposing for 2 secs, your film is _measuring_ the "bouncing, osculating"
wavefront on film. That's image BLUR. Does your site have 1/3 arc-sec
resolution, or does the recent fires at your site somewhow "increase" seeing
conditions? Or, have you found a new site, which "blows away" professional
sites like Las Palmas, Keck, etc. Let's leave the hyperbolae, while
drinking beers at the bar, OK?
I would be careful with your claims, as this is further loss of credibility
on your part.
Joe:
to answer your question, I would simply stay away from film. I spoke with a
Harvard astrophysicist, who was contemplating using film for the last solar
eclipse. The nonlinear response, made calibration far too messy. All
astronomy has gone to CCD (linear response), for ease of analysis. I think
any attempts to do any quanitative analysis for film, is a waste of time.
CCD has far greater dynamic range, negative film is limited at ~ 7 f-stops.
Film is for "pretty pictures". As a PhD, you should not be messing with
this non-scientific medium. It's for the birds..bird-brain amateurs that
is.
>
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