I always just use the smallest one. Since you get more depth of field, overall sharpness is improved greatly over larger apertures.
You DO get more DOF, but overall sharpness is not higher.
I was making the point that although absolute focus in the focal plane itself may be optimal at some moderate aperture, the greater DOF of smaller apertures can result in a sharper final images because more of the image will be in focus. That's my philosophy anyway...F/22 and be there.
I
Stopping down to f/22 (or whatever the smallest aperture is) is a way that is guaranteed to not get the best out of your lens, ever.
The effect of diffraction is quite large: possible resolution is halved (!) about every two stops the lens is stopped down.
DOF calculators are all wrong. One big fault they have is that they do not take this overall image degradation that stopping down causes into account, which makes the difference between 'sharp' and not sharp much smaller, hence DOF much larger, than the formulae suggest.
So you do get huge DOF. But never "sharper final images". Never that what you paid for when you bought the lens, never what it is capable of.
f/22, and miss out.
...
What also should not be forgotten is that diffraction always reduces what a lens can do, even at larger apertures.
Many lenses are limited by residual aberrations wide open, and the beneficial effect of stopping down will be greater than the limiting effect of diffraction. When you find the point that both aberrations and diffraction are equally bad, you have found the optimum aperture.
You have to run tests to find it. Each lens design is different, and graphs only show so much. So test.
Now if you think it worth, practically speaking, to stop a lens down to its optimum aperture, you should also not want to stop it down any further.
So forget about DOF.
Stopping down to f/22 (or whatever the smallest aperture is) is a way that i guaranteed to not get the best out of your lens, ever.
The effect of diffraction is quite large: possible resolution is halved (!) about every two stops the lens is stopped down.
DOF calculators are all wrong....
One big fault they have is that they do not take this overall image degradation that stopping down causes into account, which makes the difference between 'sharp' and not sharp much smaller, hence DOF much larger, than the formulae suggest.
So you do get huge DOF. But never "sharper final images". Never that what you paid for when you bought the lens, never what it is capable of.
f/22, and miss out.
**Interesting** - A possible source to contradict what I've been taught in Optical Theory - and proven by many moons of commercial Optical Quality Control work. Can you direct me to your source ? Hopefully it is NOT "everybody knows". [...]
... And the way to "test"? ... Optical Bench? MTF --- ?
Of course. All the lens manufacturers make *SURE* that it will be easy to *destroy* the quality of their lenses by providing easy access to "'small' apertures. They are intent on providing built-in "booby traps" for those who don't listen to "everybody knows".
But ... seriously ...
Man!!! Information about THAT progression, "halving"!!??, is something I've got to see in writing.
I hate to tell you this, but diffraction limiting is NOT directly linked to f/stops.
This is not a simple area of optical design ... you might try googling "diffraction".
No, they are not "wrong".
Uh ... can you give me the definition of "Circle of Confusion"?
f-no. resolution (line pairs per millimeter)
45 - 35
32 - 50
22 - 70
16 - 100
11 - 140
8 - 200
5.6 - 280
4 - 400
2.8 - 560
That gives resolution in lp/mm. But does it consider the large effect format size has on acceptable sharpness?
It illustrates the relation between aperture and theoretically achievable resolution.
Which is 'hard', i.e. the way it is, without anything we (including Ed) can do about it.
What resolution is still acceptable, and when, is another matter.
It depends mostly on what we find acceptable.
Criteria for CoC size traditionally are different for different formats, for exactly the reason you are thinking about.
You have been taught Optical Theory, have worked many moons in Optical Quality Control work, and do not know this?!
Now why don't you teach me how it really is?
Go on!
Take pictures.
Seriously, what have you been smoking!?
But, conveniently, from the same source, theoretical limits:
f-no. resolution (line pairs per millimeter)
45 - 35
32 - 50
22 - 70
16 - 100
11 - 140
8 - 200
5.6 - 280
4 - 400
2.8 - 560
I was going to suggest that you look up the formula that describes the relation between f-stop and resolution when posting Zeiss' table when i saw what you wrote here.
I now strongly urge you to do so!
I can. Several
One is about the thing your head seems to be spinning in right now.
Nothing you say falls into line with reality
and the fact that LF lenses are designed to be used at f22/32 and have excellent resolution across the field.
Some lens designs don't achieve edge/corner sharpness until f22m andthen how do you explain the outstanding performance of an f5.6 150mm Xenar at f32 & f45, it stops down to f64 ?
No, I DON'T "know" this!
Considering where you are starting from (and your attitude)...
Even though I am under NO obligation to instruct you in anything - you will just have to learn for yourself, I will direct you to:
This from one of the important text books:
What is Light? By A.C.S. van Heel and C.H.F. Velzel,World University Library - Library of Congress Catalog Card Number: 67-24448
Page 97, Section 4, Diffraction:
We can now turn to another facet in the study of light: the diffraction effects, the existence of which has already been mentioned. (See section 2 on the rectilinear propagation of light, and section 18 on the distribution of light at the focal plane of a lens upon reduction of the size of the diaphragm). To explain such phenomena, the great physicist and optician, Augustin Fresnel (1788 - 1827) developed a theory of the propagation of light, with which we begin our discussion.
Until now we have used as a model for the propagation of light, the theory of Huygens, which we define as follows.
One can imagine a wave front to originate out of the previous one by supposing each point in the latter to be a secondary source of spherical waves. The envelope of these spherical waves forms the new wave front..."
**Fascinating**. I will admit to having read this section a number of times, but I finally gained a fairly good "grasp" of what was going on.
Polarisation, section 5, was another matter. I passed the "tests" - but I'm still not completely sure...
Ah! Obviously an infallable way to test a lens, free from subjective judgement and preceptual bias.... NOT!
As interesting as that my be ... I doubt that it has anything to do with diffraction. Is the article available on-line ? Or ...?
The last refuge of one insecure in his argument: an "Ad Hominem" attack.
The same source? Zeiss? Now I am really interested!
Nice table. Anything to do with diffraction?
I understand some of the factors that influence lens design... What happened to "diffraction"?
Well, that really says it all. There is only ONE definition recognized as "Circle of Confusion" - an important criteria in lens design.
I]Todays high quality color films do reach resolutions in the region of 140 line pairs per millimeter with Kodak Ektar 25 leading the field at 200! The full resolution potential of these films cannot be utilized with existing depth-of-field concepts nor f-settings of f/11 and beyond.[/I]
Carl Zeiss, Camera Lens News, no. 2, Fall 1997.
I've finally reached the Zeiss website, and D'Ld the .pdf file. I see where you are coming from, but I will submit that you are extrapolating to reach an unwarranted conclusion. Here, Zeiss is commenting on theoretical limits of resolution, tied in some manner, to f/stops. I would really be interested in their methods of determining these approximate limits, but no information is provided.
According to Zeiss, a resolution of 45 l/mm (one way to look at resolution) is reaced at f/11. The normally accepted design criteria for a 35mm frame is 1/60th mm, so there will be some degradation at an aperture smaller than f/11. Notice that I wrote "some" ... the image will not abruptly disappear into a ball of "fuzz".
One thing to remember: the "practical limit" of any lens system is not entirely and wholly dependent on "diffraction"... it would be, IF the remaining parameters were all perfect... and the chances of that happening are not great.
I will ask one favor: Direct me to web site where I can find Zeiss's formula for determining "diffraction limitation". Until I can check that out, I will not continue to discuss their assumptions.
It is interesting that you consider "Diffraction" as one of the simple. basic phenomena. I think it is one or two notches above "basic".
BTW... I've been considering the "tone" and syntax of your posts ... in some way, vaguely familiar. Would you happen to be posting from St. Louis, Missouri?
Seriously, what have you been smoking!?
Ad hominem, again. You do know ad hominem means, don't you?
Go back to your books then. I bet you haven't touched them since "many moons" ago.
I hate to break the news, but, that time span is about 15 minutes.
I was going to suggest that you look up the formula that describes the relation between f-stop and resolution when posting Zeiss' table when i saw what you wrote here.
I now strongly urge you to do so!
Sounds good to me --- WHERE??
I can. Several
One is about the thing your head seems to be spinning in right now.
Hilarious. Indicative of your sharp wit, I suppose.
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