You're right. I haven't thought about the use case you describe. I think that you would be okay shooting, as you suggest, T-MAX 400 at EI 800 and push processing it. I only have data from the older TMY emulsion, but I have no reason to suspect the new one is any slower. Here's a theoretical ISO curve for KODAK T-MAX 400 (TMY) in D76 1+1. It's just a hair below ISO 400, with a very nicely linear response, but in DDX or Clayton F76+ it might be even faster.Interesting, I do shoot Tmax 3200 in good lighting when using a long lens and I want to keep the shutter speed at 1/2000 or higher and a F stop of F16 or 22. In the past I've used Tmax and DDX developer, current is Clayson F76+ which I think has many of the attributes of D76. Based on your findings if shooting in good light without a need for the higher ISO I should just shoot Tmax 400 at 800, although Kodak advises to use the same development time as at 400 maybe give it 10% more.
I am looking forward to see your results and comments.
@Andrew O'Neill I wrote the software, or, more precisely, I am still writing it. I've gotten a lot of inspiration and learned a lot from the Photrio community over the years. When it's done, I will make it available for free. Currently, it uses a command line interface and reads data from text files, but I am hoping to build a UI to work in a web browser, with some data entry and editing capability. I still have a long way go.
@Sirius Glass That's a great use case I haven't thought of. The longest MF lens I own is 180mm, so it never occurred to me that other photographers might use much longer lenses.
I think a lot of film photographers would agree that the ultimate product in photography is a fine print. Lots of criteria exist regarding what is and what is not a printable negative. Curve family and tone reproduction analyses can, to some degree, predict how negatives would print. I say "to some degree" because skilled printers can work near-miracles from badly exposed and developed negatives, not to mention the general lack of agreement of what makes a fine print. So please, take the plots below with a grain of salt.
The 13.5 min. curve (approx. EFS 1250−) of the KODAK T-MAX P3200, according to the data, seems barely printable on Grade 2 paper (Ilford MGIV FB Glossy) with a condenser enlarger and appears to be more easily printable with diffusion enlarger (or by contact printing).
Here's a curve plot of the 13.5 min. curve showing a lot of data outside of the crucial seven-zone range. Significant dodging and burning would be required.
View attachment 322236
And here's a different look at the same data, showing tone reproduction analysis of the same curve, this time, simulated with a diffusion enlarger (or contact print) and flare-resistant camera and enlarger lenses. Here, the negative is somewhat more easily printable, with some inevitable tonal compression in the shadows and highlights.
View attachment 322237
I wrote my own plotting program because I believe Phil Davis' version has too many compromises in order to bring it into agreement with BTZS. He over-simplified the camera image and tone reproduction curves. I was especially frustrated with how he calculated and depicted flare. Adding flare to the film's characteristic curve simplifies the process in that it can eliminate the need for a camera image curve. While the resulting density values can be accurately determined, I believe you lose the impression on how flare actually works. That's why I like the four quadrant reproduction curve.
In the above example, some of the numbers don't quite fit if the example is supposed to be for a normal or statistically average situation. I'm uncertain whether the flare value of 0.5 means 1/2 or is in log units. The NDR and CI is too high for a Subject Luminance Range of 2.20 to fit on a grade two diffusion. Also an LER of 1.29 is outside of what is considered grade two. It appears to be attempting to fit Zone System aims into a sensitometric model.
You might want to check out Exposure-Speed Relations and Tone Reproduction by Jack Holm. Be sure to treat his Zone System values with a little skepticism. He uses 128% for the highlight Reflectance instead of 100%.
I put something together some time ago that walks though the photographic process using the equations and plugging in values.
And something Davis never applied, here is something I wrote on the Delta-X Criterion.
You need to remember that Tmax 3200 was designed for low light work, surveillance, news, PJism, shadow detail was not a primary consideration. To understand the capacity of the film you need to use DDX, Tmax developer or Acufine. I used Acufine for a couple of rolls, was quite pleased, then Kodak pulled Tmax 3200 from the market so did not follow up.
I have not used Xtol with Tmax 3200, as a matter of fact have not used Xtol for a very long time, had a gallon of the stuff die the sudden death, then Kodak stopped making the 1 liter or quart size. Looking at the Kodak data sheet it seems that best for push is Tmax developer, Kodak lists 6400 as a push for TMX developer, but Xtol seems to a good choice as well, but is 3200 a one or two stop push? What I recall from using Tmax developer and DDX is that 3200 is not a push, which is why Kodak DX codes Tmax 3200 at 3200 and recommends Tmax developer. I found no real difference between TMAX and DDX. Different formula but I think Aucfine is a better choice for push. I just bought a quart size Acufine, I have a few cans of replenisher.
Thank you for the comments and the references! They're much appreciated. I will respond briefly, as I do not want to wander off topic, but I would be interested in discussing this in a dedicated thread, if you are willing to participate, or via DM.
Much of the knowledge resides in old journals and among enthusiasts/experts, like yourself. I do agree about Phil Davis' BTZS but I also appreciate the practical application of theory that he included in his book.
Regarding flare, I have implemented a few different methods and models so far. For example, the Phil Davis method based on the notion of "flare density" is what perhaps most photographers who read BTZS are familiar with. What I think you're referring to is the flare calculation in Quadrant 1, which is based on a "flare factor," as in Hf = (Hs * 2^F)-Hs, which is added to the camera image exposure at the film plane. Here, the flare factor, F, is in stops.
I agree that the CI is too high for Grade 2, but I wanted to include the example simulating a situation where a skilled printer can make that work. The P3200 is a film that most people, it seems, are going to push, so they're likely dealing with CI of over 0.7 most of the time.
As far as the paper data, I did this test a long time ago, so it may not be the most accurate or relevant. I should have mentioned that. I haven't yet tested the new Ilford MG emulsion, but I hope to be able to do that at some point.
Finally, you are absolutely right about mixing Zone System and sensitometric models. I haven't yet settled on how I want to do this. I want to find a way to present sensitometric data in a way that makes sense to film photography practitioners, many of whom use the Zone System. I need some advice and feedback from photographers regarding this issue because, frankly, I am stuck. Here's how Phil Davis did this in Win Plotter, as a quick example. It's not my favorite because I don't think it's very effective in conveying the message.
View attachment 322248
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