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Itsure is. Depending on the contrast between the fine detail you want to seperate there is not a definite 'limit' were resolution is lost. The diffraction 'limit' is only an recomendation. Raylegh found his limits for very contrasty objects in an experimental way. Other sample lower contrast detail and have to use a different CoC.You completely misunderstand me. For typical CoC, diffractionThat was very pessimistic. Some supertele primes and a few zoomsFor 35mm systems diffraction limits are typically around f/22, but
it all depends on the situation. If you are shooting very fine
grain film and want maximum detail you should use a smaller CoC and
therefore choose a larger aperture. But then you are very limited
in what lenses you can use to get that detail through the glass.
have its sharpest setting at wide open. Very far from F22.
limits to resolution are hit at f/22 on 35mm systems. At larger
apertures (i.e. f/16, f/11, f/8, ...) diffraction is not a factor
in resolution limit.
And there are alot of nice stuff around F5.6-F8, diffraction limited.My comment on very fine grain films is that assuming you want max
detail you should choose a smaller CoC, therefore diffraction
starts becoming a bother sooner, so you've got to find a lens that
pretty darn sharp wide open (or close to it).
Correct and I've never stated the opposite. Aberrations limit up to around F4 and at F8 it's definitely diffractions that limit quality om 'my' best lenses for resolving details at many tens of km away. Apertures at 40+cm for 35mm film and 1"- 'video', diffraction limited.Resolution limits at max aperture (i.e. f/2.8, or whatever) aren'tNja, See above.But typically, camera lenses at max aperture are not diffraction
limited. I hope you agree with that.
typically due to diffraction, they are from lens aberrations.
I think we are a bit off topic here and I'm not sure we are on the same page. Maybe we can try to convince eachother why astronomers have/use big telescopes somewhere else.It sure is.There's a lot of faint stuff out there so getting more of that
"blury" light is a good thing![]()
Correct so far.Let's just agree on the fact that there are a lot of telescopes and
most are not operated close to their difraction limit, but rather
at the seeing limit.
Nope, investments and research is made in resolving power, notSo the reason to use a bigger telescope rather
than a small one would be to gather more light. An often bigger
problem than resolving something is to get enough light from it.
increase light intake.
There are 'cheap' and very simple ways of collecting more light but
they are not used. The money is put in other investments instead.
For instance it would 'only' cost twice the money to increase
light-gathering capacity 2x times by simple renting two telescopes
and letting them track the same object. You could even avoid some
atmosferic turbulance that way and have a small resolution
advantage.
Instead of doing this, reaserches tend to just use one telescope
and increase exposures/time instead.
When more then one telescope is used it's to increase resolving power.
If light-gathering was the primary problem we would have many more
small-aperture telescopes looking at the same objects at the same
time.
If we had enough resolution vs light-gather we would:
They could save money if they scimped on quality if light-gathering
- not have single huge telescopes with hideious expensive mirrors.
was the problem, instead the mirror now stand for about 90% of the
total system cost for a big aperture telscope. Including buildings,
cameras computer HW and SW develpment.
cameras.
- not hazzling with adaptable mirrors or 10% efficient high speed
benefits too. No atmosferic absorbation of certen wavelength etc.
- Try out baloons, planes and go into space. Space have other
earth... and plan on the same thing for space.
- not invest in extremely complicated interferometer arrays on
--
Henrik
It seems that many otherwise intelligent and knowledgeable people
on this board still “believe” in the myth of the Focal Length
Multiplier (or FLM). It should be called the Cropping Factor and
that is ALL that it is.
Hopefully you meant "don't" hesitate to ask - And therefore I will ask.It seems that many otherwise intelligent and knowledgeable people
on this board still “believe” in the myth of the Focal Length
Multiplier (or FLM). It should be called the Cropping Factor and
that is ALL that it is.
--Hopefully you meant "don't" hesitate to ask - And therefore I willIt seems that many otherwise intelligent and knowledgeable people
on this board still “believe” in the myth of the Focal Length
Multiplier (or FLM). It should be called the Cropping Factor and
that is ALL that it is.
ask.
Do you have any recipes for eating crow? My dog of course, is quite
content to let the crow marinate in the sunshine, modified only by
rain, and the kindly flys that deposit their children as a spice.
But personally, having witnessed my dog happily eating HIS crow, I
was wondering if you had a better recipe?
Thanks in advance...
Dave
Hey, at least I can thank you for getting me to learn about microscopes. It's been fun reading.Thanks in advance...
Dave
That's why the very first lesson in any technical education is to be precise in the definition of terms. This thread is a good example of why that is so.I can hardly believe such a long list of posts on such a banal
topic. The only thing unfortunate or imprecise is the language we
use to describe the phenomenon. But I think most people understand
Thanks--but from both of the pages you linked to I see that numerical aperture grows as the 'objective' focal length is decreased--that is, as you put the lens closer to the object.Well - from what I've been able to understand, it's correct - asReally? That I would like to hear about!I've had a long discussion with Dave (Chato), and I think I
understand his position - more or less. He read some papers
(mostly about microscopes), and learned that a microscope's
resolving power grows with the focal length of the lens.
far as microscopes go.
With microscopes, we're talkng about the objective focal length.
That is, the distance from the object to the lens when the lens
is focused on the object . As opposed to regular focal length
(the distance from the focal plane to the lens, when the lens is
focused on infinity).