Arvee
Member
I'm finding conflicting information on this subject and hope someone can supply confirmed numbers:
Kodak says something like a CI of .58 for diffusion and .43 for condenser, a recommendation of 30% less development for a condenser enlarger (point source?),
Roger Hicks says something like a G-Bar of .62 for diffusion and .57 for condenser/diffusion, about a 10% reduction in development,
and there are other numbers in between floating around out there. I realize that G-Bar and CI are virtually identical but derived slightly differently.
I also realize these are starting points and I can find a workable number empirically but I would like to know if there is a reference(s) one can hang his hat on?
What are the recommended G-Bar/CI (or density) numbers for the following:
Diffusion/Cold light enlarger,
Condenser/diffusion (condensers with opal glass, which most condenser enlargers are),
True condenser (point source)?
And what is the reference/source of your information?
And, how valid is the old practice of reading a neg when placed on a printed page and observing a negative density of .8 when one can barely read the print through the densest part of the neg, which would be suitable for condenser enlarging?
And it also states a density of 1.1-1.2 (print just barely visible but not legible through the neg) are the target numbers for diffusion enlarging.
This practice is referenced by Phil Davis in BTZS, I have forgotten which edition.
I don't have a densitometer. I print with both diffusion and condenser/diffusion enlargers.
In college, we used the old Kodak 1A and went for a max density of 1.05 for Omega D2 enlargers, but I seem to recall that prints were typically 'hot'.
I need some idea of what the present day standards/recommendations are for each enlarger type.
Help, someone, please!
Thanks!
Kodak says something like a CI of .58 for diffusion and .43 for condenser, a recommendation of 30% less development for a condenser enlarger (point source?),
Roger Hicks says something like a G-Bar of .62 for diffusion and .57 for condenser/diffusion, about a 10% reduction in development,
and there are other numbers in between floating around out there. I realize that G-Bar and CI are virtually identical but derived slightly differently.
I also realize these are starting points and I can find a workable number empirically but I would like to know if there is a reference(s) one can hang his hat on?
What are the recommended G-Bar/CI (or density) numbers for the following:
Diffusion/Cold light enlarger,
Condenser/diffusion (condensers with opal glass, which most condenser enlargers are),
True condenser (point source)?
And what is the reference/source of your information?
And, how valid is the old practice of reading a neg when placed on a printed page and observing a negative density of .8 when one can barely read the print through the densest part of the neg, which would be suitable for condenser enlarging?
And it also states a density of 1.1-1.2 (print just barely visible but not legible through the neg) are the target numbers for diffusion enlarging.
This practice is referenced by Phil Davis in BTZS, I have forgotten which edition.
I don't have a densitometer. I print with both diffusion and condenser/diffusion enlargers.
In college, we used the old Kodak 1A and went for a max density of 1.05 for Omega D2 enlargers, but I seem to recall that prints were typically 'hot'.
I need some idea of what the present day standards/recommendations are for each enlarger type.
Help, someone, please!
Thanks!
Last edited by a moderator: