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Direct carbon on glass process

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AndrewBurns

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Hey all, first off I'm making this thread here because this alt-process area of the forum seems the most active, although my process is not 100% analogue and so I don't know if this should be put into the hybrid area. Technically this could be done in a purely analogue way and the thread is more about the chemistry of the process rather than the method of exposure, so I figured it would fit.

As you may know I've been playing with a UV projector/enlarger for a while now and one aspect I've been keen to explore is making exposures through a sheet of glass, which is something you can't do with a contact-printing process without introducing a lot of blur from light diffusion through the thickness of the glass (unless you had a perfectly collimated light source).

I've tried this with PVA-SbQ so far and it works well, although the process of coating the glass with the PVA-SbQ emulsion doesn't work nearly so well yet which is why I'm looking at carbon. I'm calling this a direct carbon process rather than carbon transfer because there is no transfer, I pour the carbon glop directly onto the glass sheet, expose the image through the glass so that the gelatine hardens from the glass surface upwards, and then develop the glass plate in hot water, leaving only the layer of gelatine that hardened onto the glass surface.

I figured that this technique might allow me to side-step some of the issues with the tonal threshold of continuous-tone carbon printing, particularly when using DAS as the sensitiser like I am. My theory is that the very thin layers of hardened gelatine making up the highlights of a normal carbon transfer print, which are likely to break away and be lost during the image transfer or development, are more likely to stick around in this technique because they're hardened directly onto a rigid support and are never put under any mechanical stress. So far I think my results are promising, although I don't think I'll completely eliminate it (but hopefully move it high enough up the scale that it's not an issue).

Here's a test print of my best result to-date, backed by a piece of white paper. Ignore the few bubbles and specs of dirt that managed to land on the print during development... The tonal scale is a bit dark-heavy and needs an adjustment to be linear, impossible to know if this is related to my process or a characteristic of the LCD screen in my projector.

_DSC5097.jpg


The dmax is not particularly great, and this is the issue I've been struggling with the most. I've tried increasing the pigment concentration, which seemed to make things worse. I tried decreasing the gelatine loading while keeping the same amount of ink to make a very thin high-contrast tissue and that also didn't seem to work. This most recent attempt was made with the following recipe:

(Wet percentage values)
10% Gelatine
2.5% Sugar
1.2% Pebeo indian ink
0.3% DAS
86% Water

Poured to a wet height of between 1.2 and 1.5mm thick (basically as thick as I could using surface tension, to go thicker would require some dams).

My UV source is about 380 nm, which should have reasonable penetration into the glop. I've tried a range of exposures and it seems that the dmax just plateaus at a certain point, like the gelatine only hardens to a tiny fraction of the total layer thickness. Before developing the dry glop layer is basically entirely opaque so if I managed to harden through most of the thickness my dmax should be very high. I'm suspicious that the problem is due to the low power of my UV projector (current exposure time for ~8x10" is 40 minutes), possibly there's a certain threshold for UV energy below which the DAS just can't harden the gelatine no-matter how long you expose it for, in which case I'm not sure what I could do. The low dmax is particularly bad if you try to back-light the glass, because then the light only travels through the pigment layer in one direction, as opposed to when you put the glass on a piece of paper and the light has to travel through the pigment twice (once to get to the paper and once when reflecting back off the paper).

Here's the same glass but backlit by an LED pad, as you can see the contrast is much lower.

_DSC5098.jpg


My eventual goal for this process is to create 4 different glass plates of a single image, each with either the C, Y, M or K layer of a colour separation. I'll then stack these glass plates on top of each other and backlight with LEDs. I think that this could result in an interesting effect where the colour layers combine to create a correct-looking image when viewed straight-on, but shift relative to each other when viewed from different angles. I'm hopeful that this will allow me to deal with lackluster dmax, as the shadows of the final image will be built up of 4 different pigment layers rather than just one and so should have much higher optical density.

Any thoughts on ways that I could improve my shadow density? Every other aspect of the process is super nice and easy, without having to transfer the image between substrates there are a lot fewer steps and a lot less to go wrong.
 

koraks

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Very interesting experiment and the results so far are quite promising, although it has to be said that even with DAS it's quite easy to get this tonal threshold behavior (with this dmax) even with a normal transfer process. Things get tricky if you want, as you're trying, to expand the tonal scale into a higher dmax.

It's difficult for me to get a feeling for how much UV power you are actually dumping into the tissue as I've only used contact-printing processes. What's your typical exposure time for a classic cyanotype with this same setup? Maybe that gives a basis for comparison.

Every other aspect of the process is super nice and easy
Yeah, there's a lot less fuss if there's no transfer. Although there are some more minor things to iron out and they might be quite challenging as well. For instance, I see that the tonal threshold on the top row starts one patch to the right of that on the lower rows. This suggests to me the tissue is thinner in that place; i.e. the glop wasn't poured to a constant thickness across the plate. Especially when doing color this will become a problem; in monochrome it's not a major issue unless you use that part of the plate for linearization. I can also see some 'waviness' in the mid-grey tones suggesting either problems with the pigment dispersion or perhaps simply artifacts from spreading the glop around during coating (or both).

For higher dmax, I wonder if 380nm will cut it. I personally use 365nm for highlights and 395nm for the black point; I've not tried any in-between wavelength. I'm not sure how feasible it is to swap in a longer-wavelength light source?
 
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AndrewBurns

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It's difficult for me to get a feeling for how much UV power you are actually dumping into the tissue as I've only used contact-printing processes. What's your typical exposure time for a classic cyanotype with this same setup? Maybe that gives a basis for comparison.

For classic cyanotype at this size I'd probably be doing a 30 minute exposure.

Yeah, there's a lot less fuss if there's no transfer. Although there are some more minor things to iron out and they might be quite challenging as well. For instance, I see that the tonal threshold on the top row starts one patch to the right of that on the lower rows. This suggests to me the tissue is thinner in that place; i.e. the glop wasn't poured to a constant thickness across the plate. Especially when doing color this will become a problem; in monochrome it's not a major issue unless you use that part of the plate for linearization. I can also see some 'waviness' in the mid-grey tones suggesting either problems with the pigment dispersion or perhaps simply artifacts from spreading the glop around during coating (or both).

I don't think that's the case. In this test print each row has a scale running from left to right, but each row is slightly different to the next, with the top row being on average slightly lighter than the bottom row. So you could imagine the tonal scale stating from top left and going down the column until the bottom and then continuing at the top of the next row, all the way until the patch at bottom right. I
would expect the first step of tone to appear on one of the rows before the others.

For higher dmax, I wonder if 380nm will cut it. I personally use 365nm for highlights and 395nm for the black point; I've not tried any in-between wavelength. I'm not sure how feasible it is to swap in a longer-wavelength light source?

I do have a 395-400nm LED module the same size and power as the 380-385nm one I'm currently using, but to swap it in and out easily I'd have to have another water cooling block machined up and to put some quick-connects in the cooling water lines (not that hard to do, and something I should probably do).

Ages ago when I was using my contact printing setup with a 405nm light source to perform 'normal' carbon transfers I was having relatively poor dmax as well even with very long exposure times (about 3 times as long as classic cyanotype with that setup) however at the time I assumed the very long exposure and poor dmax was a result of 405nm really being too long for DAS.
 

koraks

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For classic cyanotype at this size I'd probably be doing a 30 minute exposure.
Okay, I would agree with your analysis that the main problem is likely just a lack of sheer UV power density at the exposure surface. For comparison: with my 365nm light source, classic cyanotype is something like 2-3 minutes and the highlight layer for DAS carbon takes about the same up to maybe one stop more. However, the shadows layer at 395nm easily involves 10 minute or longer exposures at a similar electrical power level (both 100W lensed COB LEDs).

each row is slightly different to the next
Thanks, that explains it well.
Still, keep an eye out for any slope-off in density towards the edges of the tissue. That one has bitten me several times before and it's frankly very difficult to resolve entirely, without resorting to just not using a large rim around the center of the tissue.

the very long exposure and poor dmax was a result of 405nm really being too long for DAS.
Perhaps, although I'd be surprised if the difference between 395nm and 405nm would be so dramatic. Then again, even at 395nm it takes a heck of a lot of power to get good shadows; see above.
 
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AndrewBurns

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Okay, I would agree with your analysis that the main problem is likely just a lack of sheer UV power density at the exposure surface. For comparison: with my 365nm light source, classic cyanotype is something like 2-3 minutes and the highlight layer for DAS carbon takes about the same up to maybe one stop more. However, the shadows layer at 395nm easily involves 10 minute or longer exposures at a similar electrical power level (both 100W lensed COB LEDs).

Do you think that there is some kind of non-linear behaviour in DAS hardening of gelatine? I've seen it stated a few times (by Calvin amongst others) that you 'need' a certain amount of power per area of gelatine for DAS carbon to work at all. In a linear system you'd expect exposure to add up regardless of how little energy you're using (like cyanotype for example seems to still work even when the UV light source is weak enough you have multiple-hour exposures). However if there was some kind of threshold energy to start the reaction I could see how hours of weak exposure may make zero difference, which would explain what I'm seeing. Kinda like reciprocity failure in film I suppose.

I could see how that might put a hard limit on density, because the energy penetrating into the gelatine layer will get weaker the deeper it penetrates, and if at some depth the energy drops under the threshold needed to harden the gelatine then the top layers would continue to expose with time (resulting in darker highlights and midtones) but the shadows would just peak at a certain density and never get any darker.

I think this matches what my testing has shown. I think my only option is to try to make the gelatine layer thinner with a higher pigment loading, but then more pigment is more opaque to UV and so I'm back to square one again.

This ultimately might mean for my purposes I'll need to go back to PVA-SbQ instead, which doesn't have any issues with exposure depth or UV energy but has proven significantly more difficult to get an even coating on glass. Gelatine is really nice in that it sets long before it dries, and when it sets it 'locks' in place the local thickness and pigment distribution. PVA on the other hand stays liquid and mobile as it dries, and I've seen that uneven drying (practically unavoidable on a big plate) results in emulsion and pigment being 'sucked' from the drying areas into the wet areas, leaving very uneven layers.

I wonder if a mixture of DAS gelatine and PVA-SbQ together could work, they're both water-based mixtures at least...

Thanks, that explains it well.
Still, keep an eye out for any slope-off in density towards the edges of the tissue. That one has bitten me several times before and it's frankly very difficult to resolve entirely, without resorting to just not using a large rim around the center of the tissue.

I'll keep an eye on the tissue thickness, I also know that my projector has a pretty defined vignette which I've partially compensated for in software but I could see how that will create extra issues when trying to print colour.

Perhaps, although I'd be surprised if the difference between 395nm and 405nm would be so dramatic. Then again, even at 395nm it takes a heck of a lot of power to get good shadows; see above.

Yeah your experience of needing 4 or 5 times longer for 395nm vs. 365nm sounds like what I'd expect.
 

koraks

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Do you think that there is some kind of non-linear behaviour in DAS hardening of gelatine? I've seen it stated a few times (by Calvin amongst others) that you 'need' a certain amount of power per area of gelatine for DAS carbon to work at all.
Yeah, I've often wondered about the same, but I can't offer a firm conclusion on it. But my gut feeling is that this is indeed the case. Indeed, you'd expect exposure vs. density to be a fairly linear relationship, but things appear to be fuzzy at both the bottom and the top ends of the curve. At the bottom end, I suspect that the gelatin matrix just doesn't hold together well enough, causing total failure of the matrix to survive the warm water bath. At the top end, we have to contend with the self-masking behavior of the sensitizer; an effect that's particularly strong with DAS.

I think my only option is to try to make the gelatine layer thinner with a higher pigment loading
Increasing pigment load is the logical thing to do, yes. But at 12% ink load of your dry gelatin weight you're in a place where you should be able to get good density at least for a reflective print. For transmission density you'll certainly have to increase the pigment load - lots.
 
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