Does it make sense to discuss a proposed (but never implemented) change to the speed criterion published by C.N.Nelson in 1959, based on a standard from 1954 or even earlier? Back then, unlike today, films had an extremely S-shaped densitometric curve.
I just want to first make a few factional corrections before moving forward.
On page 443 of Theory of the Photographic Process, 3rd edition.
The Delta-X Criterion is discussed for 1 1/2 pages. Towards the bottom of page 443.
“In view of the data presented by Nelson and Simonds, it is clear that the poor correlation which Jones and Nelson found between speed numbers obtained from the D=0.10 criterion and speeds obtained from a statistical determination of the “first-excellent” print can be attributed to the use in their investigation of negatives that had been developed to widely different average gradients.”
And on page 444, “It is now feasible to restrict the use of the speed criterion to those cases in which the negative material is developed to a fixed average gradient corresponding to that realized in commercial practice. With this restriction incorporated in the development specifications, it follows from the studies of Nelson and Simonds (Simple Methods for Approximating the Fractional Gradient Speeds) that the fixed-density (D=0.10) speed criterion is a valid correlate of the fractional-gradient criterion.
In 1957, the responsible committees of the American Standards Association undertook the drafting of a revised American Standard Method for Determining Speed of Photographic Negative Materials (Monochrome, Continuous Tone). One of the primary objective in writing the standard was to specify a method of testing which would permit the use of a fixed-density speed criterion. The view was held that by abandoning the fractional-gradient criterion, which had been specified in previous American Standards, and adopting a fixed-density criterion, a serious obstacle in the way of international agreement on the method for determining speed would be removed. Because, in addition, the use of a 0.10 fixed-density criterion in combination with a suitable development specification offers the convenience and precision characteristic of this criterion and retain the practical significance of the fractional-gradient criterion, this method was adopted in the new American Standard."
I’ve found papers explaining the theory behind a new photographic standard were common, like Safety Factors in Camera Exposure. Some of the papers could be about proposing a change to a standard, but as Safety Factors was published in 1960, the same year as the new speed standard, and the above quote has the committee working on the new standard in 1957, it appears it was at least being written concurrently with the standard. So, for a better understanding of the choices in the ISO speed standard, two of the papers one should read are Safety Factors and Simple Methods of Approximating the Fractional Gradient Speed.
Other reasons why I think ISO 6 is outdated and no longer useful:
As for being outdated, the standards are reviewed every 5 years. While the ASA standard was later adopted as an ISO standard in 1974, and then revised in 1993, the changes were primarily methodological and didn’t change the core theory. It has not been revised since.
Modern films have a more or less straight line that starts at zone II (maybe II-III) and goes beyond zone X. Applying the ISO process to such films results in a high contrast gamma of about 0.7. ISO film speed is thus based on N+1 push development. For this you would need multigrade paper with grade 0.5, but normal contrast should fit on grade 2!
ISO places the speed point in the flat toe of the curve in zone I with a density of 0.1 over base+fog. This was a compromise that still exists today in ISO 6. The base of the density curve below D=0.2 is of no interest for practical photography, as details are no longer resolved. Many large-format photographers tend to place the shadows in zone III with a density of at least 0.35. The film density in zone I is ultimately irrelevant.
There's a lot to unpack in there. I'm going to ignore the Zone System stuff as that has more to do with metering and setting an EI than the ISO speed standard. There are a few points I'd like to make. As I said in a previous post, the ISO parameters produces a film with a gradient of 0.62 especially in the case of short toed films. Because gradient is calculated as Rise / Run, the length of the run and how it relates to the film curve is important. In another thread, I should how the value of the gradient can change depending on the type of film curve and the length of the run. As the ISO standard uses Δ1.30 for its run, developing a long toed curve to a ΔD = 0.80 tends to produce a negative with a CI higher than 0.62. I emphasis once again the standard isn't suggesting this is how to process a pictorial negative. It is used for the speed determination of the ISO standard, so much of the point in the first paragraph moot. Considering a normal negative to be contact printed or printed on a diffusion enlarger is considered to have a CI of 0.58 based on a paper LER of 1.05, Luminance range of 2.20, and 0.40 of flare, a CI of 0.62 is about 1/3 more contrast as stated in a previous post.
A good paper that addresses print quality from different film types is Simonds, J.L.,
Factors Affecting the Quality of Black-and-white Reflection Prints, The Journal of Photographic Science, Vol, 11, 1963.
As for density being a deciding factor in exposure placement, there's a favorite quote by Lyod Jones, "From the standpoint of tone reproduction theory, there seems to be no justification for the adoption of any value of density as a significant criterion of the speed of a photographic negative material. The primary function of the negative material is to record brightness differences existing in the scene. Density, per se, has no significance as an indication of the ability of the photographic material to perform this function. The value of negative density by which any particular object brightness is rendered, as, for instance, the deepest shadow, is of no consequence except insofar as it may have some bearing on the exposure time required to make a print from the negative."