> OK, so I reviewed this - and I understand some of the logic you use, but I have to admit it makes no sense to me in real life.
It will soon.... remember, the f #'s and their MP's are MAX. POSSIBLE recorded resolutions, not min. resolutions. This also represents the resolution at the POF (Point of exact Focus). So this assumes you are shooting a FLAT test target or an infinity scene, both having a flat focal plane. When you introduce depth into the equation, the near and far points will always have less resolution than the POF, (up to a point) so the f# and MP's values I offered above, you can cut them by 20 - 50% (estimate) based on the amount of depth you have in a scene. This is why the 568 MP values are so far from reality.... real world depth MP values for 8x10 at f45 can be in the 40 - 90 MP range, based on the amount of depth and f stop used. (more on this below) There has been several web examples of 40 MP digital captures nearly matching 8x10 film - same composure being compared...(color, not B&W) .... and when there is enough depth in the scene the gap can be surprisingly small...but shoot infinity subjects or FLAT subjects, and 8x10 film will destroy a 40 or 60 MP back. This is why the comparisons are all over the map... the devil is always in the details....
Also, as per my f# vs. MP values above, ..... in the real world, nothing is perfect, so these values are not fully attainable even with FLAT subjects such as test targets....but with enough precision, the right lenses, used at the right f stops, optimum subject contrast, optimum subject sizes, precise processing, etc., in theory they are attainable ....
Film records contrast....the finer the subject detail, the less contrast the lens will deliver, and the less detail the film can record. This is why you must combine the MTF of the lens and the film, and why they are both dependent on image frequency (amount of detail) Just look at the MTF curve of a lens, at high enough resolutions, their ability to deliver clean contrast to the film, goes right in the dumper. Bruce mentioned a perfect example, pine needles at a distance.... low contrast and very fine detail, in most cases, 1/R will turn these needles to mush on film... sad, but it's reality. It's the nature of imaging, not just film, same true with digital. But digital has the benefit of lower f stops, due to more dense recording media. This is films Achilles heel. Anyway, this is why there is some generalizations when making these "ballpark" judgements. In most cases, its to get us in the ballpark... unless you really want to get down to the sheer nitty gritty stuff...
> I recently did a test of the same image shot from f 22 to f 64. The only difference I can see is in depth of field. The sharp areas are very sharp in each one. If I read the above correctly, the f22 ought to be really superb as far as detail (at least where it is sharp) and the f64 ought to be about 1/4 the resolution - and 1/4 the file the other is. They are both very good.
As Bruce correctly mentioned .... at the POF (Point of Focus), f22 should yield a sharper image than f64. However, if the subject at the POF does not have enough detail, then it will "appear" equally sharp. The difference is, at f22, if you put finer detailed subject at the POF, then you will see how the MTF of the lens and film will yield a sharper image at f22. This where the nitty gritty comes into play. Just imagine a single metal column at the point of exact focus.... no detail....shoot at f22 and f64, it would be hard to tell the difference in the processed film....at best you will see tiny differences at the edges under high magnification. Now put a Pine Tree at the POF, you will see the difference very handily.... Of course, this is just at the POF....at the near / far points, as you suggest will vary greatly based on f stop.
> This is where I have trouble - the numbers don't match my experience.
This is because you are not applying all the variables to the equation. This is the value of performing tests with targets, it removes the subjectivity of saying, "they all look good"... with targets, you see where the cut-off is at each f stop and camera to subject distance. When done right, I can assure you after years of testing, the reality of recording detail is very predictable. But I will agree, it can be tricky for the newb... lots of variables within the optical principles and lots of variables in the particulars of specific lenses, films, etc. Again, the goal is not to nail results to within 5%....the goal is to prevent us from being off by 500%.... and thinking we are right... that's what the math is for... it steers you in the right direction for a specific task.
> I'm not trying to be argumentative. I just don't see it.
I understand you are not being argumentative...no problem. I hope my explanations helps you understand why "you don't see it" .... shoot test targets, and you will discover the basic math is remarkably accurate.
> This leads me to the conclusion that, as with many numbers, they are theoretical. Imacon is famous for claiming that they have a DMAx of 4.8, which is beyond the maximum density of film.
When doing a test, you need subjective information and must understand all the variables. From what I am reading, that does not seem to be the case here... the math is not "theoretical" it's been proven science for 50+ years. It's easy to be fooled by a test, then assume the math is faulty. I would not compare sound science like this (with no monetary motive behind the science) with Imacons marketing claims of x dpi or y Dmax. We know manufacturers exaggerate, stretch the truth, deceive, etc. to help sell products. This is a weak analogy.
> However, i have a 8x10 image, scanned at 2000 ppi I am looking at that is just over 300 mgpxels (16000 x 20000), about 500 megs of B&W and I don't see how it relates to being only 1/3 usable pixels.
The mistake you make is.... you assume the dpi you scan at - dictates the amount of resolution a given piece of film contains. You have the tail wagging the dog. The amount of resolution film contains is determined during imaging, not during scanning. I have seen you mention this several times. Here is a simple example that hopefully will bring these numbers into reality.....
We shoot a flat target at f45 with 8x10 color film with 60 lp/mm MTF at the given contrast value of the target. We assume perfect film alignment, focus and diffraction limited lens at f45, single focal plane.... OK?
AT best, we can resolve:
1/(1/33+1/60) = 21 lp/mm
(1500/45 = 33 lp/mm aerial rez)
This means a 30 lp/mm target at the film plane will NOT be resolvable under magnification...it will appear as a blob, vs. cleanly defined lines. It means 20 lp/mm target on the film will appear barely discernible....not a blob, but not sharp. A 10 lp/mm target will look sharp, and a 5 lp/mm target will look razor sharp. This is MTF at work... the finer the detail, the less contrast that is Transfered (hence the T, in MTF) This testing procedure is as old as the hills.... no voodoo math here.
Now, how much "usable resolution" does that 8x10 film have? The film has nothing resolvable over 21 lp/mm.... so it's resolution is stated as 21 lp/mm. Keep in mind, it might have areas of much less resolution, but 21 lp/mm represents the max. recorded resolution.
But since we want MP's, we must consider the film area.
21 * 2 = 42 lines per mm (not pairs)
lines in X Y axis are analogous to pixel
8x10 film is 200 x 250mm
or 10,714 * 8,571 = 91 MP
So 91 MP is the total amount of resolvable information in that 8x10 piece of processed film. No scanning is required to determine this... only a good film loupe, microscope and some simple math. It does not matter how deep you scan that film, there can not be more useful information than 91 MP. The scanner, AT BEST, will only extract the useful information in the film, it will NOT create new information. Hence why there is NO relationship between the size of your scanned files and the useful MP's in the film. Larger scanned files are due to the inefficiency of the scanner, which includes all the variables I mentioned in my previous post. Make sense now?
End of Part I
Bookmarks