Hi:
I’ve slowly been getting used to the 8x10 workflow over the last year and a half, and am now comfortable enough to take on the next technical curiosity: still lifes and macro abstractions.
I suspect a lot of people will come out and say 8x10 is a poor choice for this type of work, but I’d be curious to explore what the technical realities would be. For example, what is the smallest object that can be enlarged to 8” on the film? What would the bellows draw need to be, or rather, what’s the smallest object or area that can be photographed with the length of my deardorff V8 bellows? What focal lengths and optics are recommended for best results? My other lenses are sironar s and apo-Ronars, so sharpness should be in the near neighborhood. Or does compounded diffraction at such long bellows draw make this impossible?
Any other general thoughts?
I have some 2” figs I’d love to split in half and photograph but I don’t know if this is fantasy in this format.
Jarin
True and a good point. When a lens is listed as symmetrical they usually mean that the rear elements correct the distortions of the front group but there are a lot more actually geometrically symmetrical lenses in the large format world than there are in 35mm as you suggest. Embarrassingly the high f-stop repo lenses I mentioned are the most likely ones to be truly symmetrical. I guess you have to take it on a case by case basis. Thanks for correcting my oversight.Some universal-use LF lenses are near synmmetrically built, like the old Symmar versions. Twisting these likely has not much benefit.
I think what I might do is save up for a macro apo sironar 180mm. At around full draw on my camera (31”/787mm), this should achieve nearly the 4:1 enlargement I am after while not crushing the camera as close as a 120mm.
At 4:1, what is the diffraction equivalent/conversion to “normal” photography? If I usually try to limit myself to f/45 or less, what is the equivalent at this scale? If I am working at 5x the normal bellows draw, does that translate to a 5 stop diffraction equivalent, ie: f/8 = f/45 level diffraction?
J
Jarin, get the books I recommended. Read the books. You'll learn more that way than by asking random questions and getting random answers.
The magic formulas you need are:
effective aperture = aperture (f/ number) set * (magnification + 1). Example. f/22 set @ 1:1 is f/45 effective.
diffraction limit is approximately 1500/effective aperture.
I've heard of a technique for large format macro that uses a dark room, a sliver of light, and a table on a track. The idea is kind of like focus stacking for digital photography, only instead of shifting the focus of the camera and recombining the image in software, you keep the camera's focus fixed, light only the area in focus, and drag the subject through the slit of light. Apparently it works best with lasers instead of regular light. That way your only exposing the film to the subject while it is in focus. I've never tried it and never seen it done, so I'm not sure if I have all of the details right.
Jarin, there's no substitute for book larnin'. Buy the books and read them.Yes, I will have to look into these, although I feel like with this basic starter information, i’d Be ready to start accumulating information through practice, ie when prints start to look soft to me personally at which apertures, etc.
Thank you for these formulas. So apparently f/11 on the lens will equate to f/55 as far as diffraction and exposure (T stop). I’ve seen the other formula before, I believe to calculate lp/mm in regards to diffraction limit?
J
That's right! I seem to remember that too now. I think in the article I read, they had three projectors (maybe?), one at top and one on each side. I believe they used them to culminate the light, so that it didn't spread out so much after the slit. They didn't use the lasers for that article, but I thought I read somewhere that scientists would sometimes use them, as the light from a laser won't spread out hardly at all. But then again, it could have been because they were scientists, and lasers were easier to come by than projectors. A laser would be a terrible choice for color photography, and depending on the color of laser, it may not be a great choice for black and white. So it's probably more complicated than it's worth.Yep, sounds about right except for the laser part, I think. And it doesn't have to be large format. I first read about it in an older issue of Kodak Tech-Bits, a sort of scientific publication that was not too well known. It's been on my list of things to try out someday when I get ambitious enough.
In the article, as I recall, the author used a slide projector(s) with a narrow slit of some sort for the slide. The slit is projected so as to be perpendicular to the lens axis, so that no matter what part of the subject the light beam strikes it will be in the focus plane. I vaguely recall a macro shot of a beetle used as an example - it was crisply sharp from front to back. (Obviously the subject cannot be alive, or at least must be immobile.)
Jarin, there's no substitute for book larnin'. Buy the books and read them.
We don't speak the same dialect.You misspelled " lurnin' ".
You might could use a condenser enlarger head too [as light source for slit scan macro photography]. They culminate the light, much like a projector.
Perfectly said.You asked some apparently simple questions that want book length answers. Get the books, read the books.
It's only been on my back burner for about a year now, so I'm at least 19 years away from attempting it!Yep, this is the method I was planning to use; perhaps a couple of them. For the tracking motion, probably a cheap drill press vice with 2-axis movements ("dovetail" guides, and driven by a screw). I'm sure I would have done it by now if I had a severe interest in insects, or whatever, which I don't. So it's been on the back burner in my head for 20 or 30 years or so.
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