Geary Lyons
22-Jul-2008, 16:55
I have had several questions regarding controlling contrast, split grade printing and a simple LED VC head. I'm looking for some input and consensus.
So, the basics, VC paper uses blue versus green sensitized emulsion to achieve the overall contrast range. The papers were designed to respond to, the then available, tungsten light sources. VC filters and color dichroic filters are designed primarily for tungsten light. That is a light spectrum heavily weight on the red end and lot's of heat, (heat = infra red!).
In every dichroic head, that I have examined, the range of M or Y filtration is determined by how far into the light beam the single value dichroic filter is pushed or pulled. That is, the dichroic filters are not graduated as one might assume from the numbers on the dials.
So my theory, and the basis for my LED head, is that the variation of exposure time at green and blue is the exact same relationship as how much of the tungsten light beam is passed through the Y or M dichroic filter. If one spins the Y-M dials to max, in split grade printing, then the relationship of hard & soft contrast is exposure time based, just as in the simple LED G-B configuration. Varying the ratio of green to blue light exposure time can provide any contrast range between the two extreme produced by the LED spectrum. This theory is confirmed in Lambrecht-Woodhouse Way Beyond Monochrome, (page 79, figure 3).
So why are some folks telling me that they MUST have the ability to vary the G-B light intensity as a control function on the LED head? I can understand if they want to achieve a certain "equivalent contrast grade" overall or localized in the more traditional VC printing concept. But they are insistent that the variable density, (luminosity), of the B-G light is critical in split grade printing as well!
Am I missing something?
You thoughts would be greatly appreciated!
Cheers,
Geary
So, the basics, VC paper uses blue versus green sensitized emulsion to achieve the overall contrast range. The papers were designed to respond to, the then available, tungsten light sources. VC filters and color dichroic filters are designed primarily for tungsten light. That is a light spectrum heavily weight on the red end and lot's of heat, (heat = infra red!).
In every dichroic head, that I have examined, the range of M or Y filtration is determined by how far into the light beam the single value dichroic filter is pushed or pulled. That is, the dichroic filters are not graduated as one might assume from the numbers on the dials.
So my theory, and the basis for my LED head, is that the variation of exposure time at green and blue is the exact same relationship as how much of the tungsten light beam is passed through the Y or M dichroic filter. If one spins the Y-M dials to max, in split grade printing, then the relationship of hard & soft contrast is exposure time based, just as in the simple LED G-B configuration. Varying the ratio of green to blue light exposure time can provide any contrast range between the two extreme produced by the LED spectrum. This theory is confirmed in Lambrecht-Woodhouse Way Beyond Monochrome, (page 79, figure 3).
So why are some folks telling me that they MUST have the ability to vary the G-B light intensity as a control function on the LED head? I can understand if they want to achieve a certain "equivalent contrast grade" overall or localized in the more traditional VC printing concept. But they are insistent that the variable density, (luminosity), of the B-G light is critical in split grade printing as well!
Am I missing something?
You thoughts would be greatly appreciated!
Cheers,
Geary