I have heard that "standard contrast" for negative film is 0.6, on the straight-line portion of the h&d curve. I have a couple of questions about this.
1. is this true?
2. Why 0.6 not 1?
3. Do manufacturers development data uniformly target this standard contrast value?
4. If I have papers from grade 0 to grade 5 at my disposal, how much tolerance does that give me with regards to the contrast of my negatives?
I am trying to determine if there is a development recipe that I can use with all the different films I use.
The Kodak Xtol datasheet says that if you develop TMY for 9.25 minutes, that the contrast will be 0.56 at an exposure index of 400, but 0.62 at EI 800. Why would exposure index make any difference in contrast, at the same development time?
The low contrast value for film was chosen to give the longest latitude possible, and so that printers could select the point on the straight line for optimum printing. Or, they could use split grade or a host of alternative processes. A low contrast film would limit option. Besides which, paper has its own limiting latitude imposed by the lack of ability to go much over 2.0 in density in an enlarging paper. So, the film supplies the latitude and the paper supplies the best image possible imposed by the laws of physics.
The Kodak Xtol datasheet says that if you develop TMY for 9.25 minutes, that the contrast will be 0.56 at an exposure index of 400, but 0.62 at EI 800. Why would exposure index make any difference in contrast, at the same development time?
The ISO method of determining speed does not directly use the straight-line contrast, but rather seems to define contrast in the toe region. If I understand correctly, different films, when developed to the ISO criteria for shadow speed, may then have varying straight-line contrast. Actual photographers, on the other hand, seem obliged to develop to a target contrast that looks correct. I would be interested to know what this contrast ends up being for different films when they are developed according to the ISO standard.
1. The standard is based on the statistical average conditions and the average paper grade. Loyd Jones determined the statistical average luminance range is 2.20 logs or 7.33 stops. Now this doesn't include the entire range from accent black to a pure specular reflections. This is all based on Tone Reproduction Theory which is a fascinating subject. Kodak had 0.56 as their normal of a couple of decades, but changed it to 0.58 because of the increased use of 35mm cameras which have a slightly higher average flare than larger formats. Flare went from 0.34 to 0.40 or 1 1/4 to 1 1/3 stops. According to the below chart published in Photographic Materials and Processing, the LER that falls in the center of the range for a grade 2 paper printed on a diffusion enlarger is 1.05. This also doesn't include the entire range of the paper.
1.05 / (2.20 - 0.40) = 0.58
View attachment 101336
2. Why not 1? The negative is not the final step in the process. Paper just so happens to be slight under 2.00 (~1.70) so the negative needs to be about half that in order the reproduction to equal 1.00. negative gradient x paper gradient = 1.00.
3. Manufacturers tend to follow the statistical averages.
4. Please see the chart above and the table I've uploaded. While matching the NDR to the Paper LER helps match the film to the paper, it doesn't account for the local contrast and how the print tones relate to the original values.
Other people have already pointed out the connection between 0.60 sounding familiar and the ISO black and white film standard. The number; however, can be misleading. While it is technically processing the film higher than normal, it doesn't make a change in the film speed when you consider the standard uses the Delta-X criterion for speed determination. Delta-X is a way to mathematically determine the placement of the fractional gradient point using an easy to find fix density point. The contrast parameters of the standard are part of the math. If the negative has a density of 0.80 at a Δ1.30 log-H from the 0.10 density point, the difference between the 0.10 and fractional gradient point is always 0.296. Only when these conditions are made can you determine accurate film speed. At other film gradients, the Delta-X equation must be used. As the film speed doesn't change very quickly with changes in film gradient, the slightly higher gradient for ISO testing does not give a false higher speed value.
Illustrative curves for two hypothetical films (zero B+F density) with the same ISO speed but different toe shapes.
Thanks for the explanation. I don't think this explains the TMAX datasheet thing though. I don't see how the curve shape could be said to change if the film is developed the same. Kodak must be using a different definition of contrast index here.
The low contrast value for film was chosen to give the longest latitude possible,...
PE
The "first acceptable print" method has determined that this is the print that has little or no curvature from the film in it.
The Kodak Xtol datasheet says that if you develop TMY for 9.25 minutes, that the contrast will be 0.56 at an exposure index of 400, but 0.62 at EI 800. Why would exposure index make any difference in contrast, at the same development time?
I don't think that answers the question because it leaves the question of what is so special about #2 paper.
My research and personal experience has me understanding that rollfilm negatives have higher quality if they are processed to gammas of less than 1. So my premise is papers are manufactured to support those lower gammas. Not the other way around.
I don't know of a research paper that specifically addresses these issues (that is why I am engaging you further into the conversation) but I have inferred my above premise on tangential remarks present in some of the papers I reviewed (many of which you sent to me).
For example my premise is supported in the Nelson paper Safety Factors in Camera Exposure, 1960. There is a graphic indication of the adverse effects of extended development of enlarged rollfilms.
View attachment 101392
Here's the dilemma or paradox BetterSense is talking about.
My proofreader's opinion is that the number marked with an asterisk should be 0.56
Real quick. The first excellent print test lead to the fractional gradient method, which by it's very nature having the speed point at 0.3 time the average gradient places exposure in an area of curvature.
Stephen, these were all evolving at the same time as everyone realized that what was needed was a long latitude film and this could not be done with reversal. Everyone in design knew this and knew how to test for it to prove its reality.
The qualification needed was the ability to coat and test films and papers with different contrast gradients. I am one of the lucky few who have been able to do this (within limits - the cost burden to the project at hand), and to prove these suppositions against actual results and customer comments.
To do this, Daan would send out bundles of prints to customers for comments. Leroy would read the densities in a MacBeth viewing cabinet, and the results of comments and readings would be tabulated. And, BTW, the densities actually viewed NEVER matched those of a reflection densitometer due to angle of view (goniophotometry). Thus, all data had to be reconciled.
This is not a math problem for the head, it is a combined human - math - coating problem which must be done in its entirety in order to comprehend the actual "print space". Grant and I had the opportunity to discuss this at length during our tenure at KRL together, and we agreed (I think) that this was not just about graphs. The piles of Zwixpix that I had in my office bore testimony to that.
PE
Illustrative curves for two hypothetical films (zero B+F density) with the same ISO speed but different toe shapes.
Ron, you misrepresented the conclusions from the "first excellent print." Your statement was about a specific test.
No, I did not. I know what "first excellent print" means and in fact delineate this and related latitude in portions of my book. The first figure shows the first excellent print, but the majority of excellent prints are further up the curve or slightly over exposed from one POV. The second two figures from Haist show the effects of exposure on latitude or the effects on getting an acceptable print. These three figures are all that one needs to understand more fully, neg-pos systems.
PE
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