Pieter12
Member
I'll take a wild guess. In a projection system, the light source is at a relatively fixed distance from the lens, the projected image distance can vary much more. In a camera, the opposite is true. Maybe.
We aim to please.
I expect that there may be some additional losses due to the fact that there is a greater chance of flare outside of that portion of the lens' imaging circle that is in the frame, but that is probably trivial in amount.
Do you have to factor in bellows extension with projection???
The bellows extension calculations can actually be re-configured so that magnification is the variable that determines what bellows extension exposure compensation is required.
As the magnification is the same in the two examples - full frame with a 50mm lens, and full frame with an 80mm lens at a higher elevation - there is no change.
Do you have to factor in bellows extension with projection??? I have no idea.
I have a application on my Android phone that I use to calculate f-stop times. I also have F-stop timers on some of my equipment.
Of course with the old wonderful Cibachrome, Ciba recommended using a constant time and changing the aperture, the ultimate in f-stop control![]()
Thats how i thought f stop printing worked...
Changing f-stops can change focus.
Changing f-stops can change focus.
Changing f-stops can change focus.
and originally i thought that Fstop printing was a theory to regulate aperture size and "light exposure time" via timer settings... as a means to figure out a way to save paper and scale an enlargement between paper sizes
TRUE, but the focus knob is really easy to use,, but getting the image resized can be a pain in the cheeks..
Changing f-stops can change focus.
Changing f-stop was recommended by Ciba and later Ilford with Ilfochrome because of the reciprocity characteristics of the print material. Color shifts, unpredictable density etc.
Holds true for RA4 processing, also. At least for the color shifts, which I experienced trying to do a simple burn in a corner of the sky.
As you have probably gathered, f-stop printing should probably be called "stop" printing, because exposure adjustments are done in increments of stops and fractions of stops, rather than in linear increments.
But calling something "stop printing" would just confuse everyone!
If one had the ability to repeatedly and reliably adjust the lens aperture in 1/2, 1/3, 1/4 or 1/6 stops, one could approach f-stop printing that way.
In contrast, it is quite easy to make those sorts of adjustments in the exposure time, if one has the appropriate enlarging timer.
In theory such an enlarging lens COULD be designed and built...
and originally i thought that Fstop printing was a theory to regulate aperture size and "light exposure time" via timer settings... as a means to figure out a way to save paper and scale an enlargement between paper sizes
In answer to the question posed at the end of post #44
The actual shutter times in seconds are: 1, 1/2 , 1/4 , 1/8 , 1/16 , 1/32, 1/64, 1/128, 1/256, . . . consistent with the law of reciprocity.
These are the reciprocals of 2 to the integer powers 0, 1, 2, 3, etc.
The apparent “jump” after 1/8 second is simply the result of the convention used by camera and shutter makers to give a sequence of denominators that end in 0 or 5.
There are no shutter times of 1/15, 1/30, 1/60, 1/125, . . It’s merely a convenient fiction. It does no harm. Likewise, the familiar aperture number sequence 1, 1.4, 2, 2.8, 4, 5.6, 8, 11, 16, 22, . . . is a result of convention.
The even powers of 2 give exact values 1, 2, 4, 8, . . . The odd powers of two rounded to 1 decimal place give 1.4, 2.8, 5.7, 11.3, 22.6, 45.3, 90.5, and so forth.
By convention, the value of f/5.7 is truncated to f/5.6 while the remaining values of the odd powers are truncated to integer values 11, 22, 45, 90, etc.
Or wonder how long it takes for the electric powered aperture to get out of sync due to wear and tear...
Surprisingly long. If you look at how common such apertures are on lenses that have been in common use since the late 1980s, many of which have seen heavy abuse, it's really remarkable how incredibly few have failed or drifted in such a way to become problematic.
How do i hack the aperture control system to leave the shutter open non stop...
The aperture is not the shutter, so why would it help to try hacking the aperture control system to do something with an unrelated shutter that's not present on the majority of enlargers anyway? On a non-existent electronically controlled aperture enlarger lens, no less?
Edit: but perhaps I misunderstood your question, and what you intended to ask was "how would one get a suitable 50mm camera lens with electronic aperture to stop down to the desired aperture when bolted onto an enlarger?"
One possible way is by starting with a Canon EF lens, since the EF mount uses an industry-standard SPI interface and the aperture control commands have been reverse engineered an published years ago. One could hook up a microcontroller and any desired user interface to the lens and writing a program that controls the aperture. Aperture control in these lenses consists of a tiny electromotor that can run in opposite directions - one direction for opening up the aperture, and one for stopping down. Control is done by running that motor for a set number of microseconds to get the desired aperture. This is not too difficult to manage for someone with some experience with embedded systems. I.e., someone with moderate Arduino capabilities could hack something together that will work.
With non-Canon lenses, the same mechanism can likely be exploited, but you'd either have to reverse engineer the brand's proprietary mount communication protocol. But personally, I'd just hack the lens a little further and directly drive the aperture motor instead.
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