Re: Using a 660nm laser to expose legacy AgX Agfa, Ilford, HRT (BB) plates
Posted: Fri Apr 08, 2022 9:53 am
The curve in the post above is not exactly the true picture, as it is a graph of relative sensitivity, not absolute, unlike this curve, from Agfa Technical Information Bulletin 21.7271(688)LI, the rest of the bulletin available here: http://edweslystudio.com/Materials/AgX/ ... 271688.PDF
The absolute sensitivity never falls to zero, just varies over the spectrum, with that area that is the borderline between blue and green, cyan, where the 488 nm line of the Argon laser reigns supreme, is where it dips to its lowest value. The guidelines were put in place to show that the difference between the sensitivity at the He-Ne red of 633 nm is about an order of magnitude greater than that at 488 nm, almost 10X, or about 3 or 4 photographic stops, which are binary orders of magnitude, which is borne out in practical experience.
The -2 on the ordinate (vertical axis) could be translated as 100 microJoules/cm^2, and the -3 as 1000 microJoules/cm^2 or 1 full milliJoule/cm^2, since the axis is logarithmic. These figures are again borne out in practice, as 100- 200 microJoules/cm^2 is usually the bracketing point when I make test exposures at red wavelengths.
Comparing the 2 graphs, the shape of the curve is the same, but the numbering of the relative's ordinate, which is also logarithmic, starts at zero, and ascends as powers of 10, and once again it can be seen that the sensitivity difference between the 2 lambdas is an order of magnitude off. The drawback to the relative graph is that it gives an impression of absolutely no sensitivity, but the zero in a log axis is 10^0 = 1, so that dip is used as unity, the standard of comparison, not as an exposure suggestion.
The absolute sensitivity never falls to zero, just varies over the spectrum, with that area that is the borderline between blue and green, cyan, where the 488 nm line of the Argon laser reigns supreme, is where it dips to its lowest value. The guidelines were put in place to show that the difference between the sensitivity at the He-Ne red of 633 nm is about an order of magnitude greater than that at 488 nm, almost 10X, or about 3 or 4 photographic stops, which are binary orders of magnitude, which is borne out in practical experience.
The -2 on the ordinate (vertical axis) could be translated as 100 microJoules/cm^2, and the -3 as 1000 microJoules/cm^2 or 1 full milliJoule/cm^2, since the axis is logarithmic. These figures are again borne out in practice, as 100- 200 microJoules/cm^2 is usually the bracketing point when I make test exposures at red wavelengths.
Comparing the 2 graphs, the shape of the curve is the same, but the numbering of the relative's ordinate, which is also logarithmic, starts at zero, and ascends as powers of 10, and once again it can be seen that the sensitivity difference between the 2 lambdas is an order of magnitude off. The drawback to the relative graph is that it gives an impression of absolutely no sensitivity, but the zero in a log axis is 10^0 = 1, so that dip is used as unity, the standard of comparison, not as an exposure suggestion.