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- Jan 17, 2013
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- Holga
Eastman-Kodak had false curve toes with their black-and-white reversal films PXR and TXR. Actually, the entire curve was simply shifted out of the base density of log 0.23 in order to pretend clear lights.
Retro...
The sheets can be used that way. The vertical height of the curve is the response in LogE. The "Y" axis is thus the speed at that wavelength. However, the speed is the integral of the entire curve. And so the speed that you measure at one wavelength is infinitely small regardless of the "Y" value unless combined with all of the other values.
This all is related to calculus, I'm afraid. And, the curves have to be smoothed out because they are bumpy due to the dyes themselves.
It is easier for a B&W film than for a color film, due to overlap. Thus, some green light produces red exposure. How do you estimate that? You need to do spectral curves of each dye formed at each wavelength and then begin to calculate what must be done to improve color reproduction.
To do that, you must also include a factor for the human eye vs the measuring system, and you must therefore consider the half band width of the imaging dyes.
If I can find one, I might post a typical picture used for this type of measurement.
PE
May I ask, to what practical application will the OP put a perfect interpretation of these spec-sheet curves?
It's not meant to be a silly question, as all that consistency necessary thirty years ago - when film was the starting point for many analogue image-production processes - seems to have been removed. Now aren't we are using consistency in our own personal processes to achieve what we want at the level of an individual print (or small, personally repeatable, batches), not as the start of a long chain of analogue processes where the published result depends on perfect global consistency at every step?
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