Originally Posted by
Leonard Evens
The point about the hyperfocal distance is that if you focus at that distance, in principle, everything from half that distance to infinity will be in focus. If you focus in front of the hyperfocal distance, your depth of field won't extend to infinity. If you focus at greater than the hyperfocal distance, your near focus point will be further out than necessary.
Of course, hyperfocal distance depends on the f-stop and your criterion for sharpness, i.e., your maximal acceptable circle of confusion. It is also calculated for a perfect lens and ignores diffraction. So, in practice, it is at best a rough guide. When I use such methods, I focus at the calculated distance and then stop down from half to a full stop further.
The hyperfocal distance is given by a relatively simple formula
f^2/(Nc)
where f is the focal length, N is the f-number, and c is the maximal acceptable circle of confusion. A reasonable choice for c for 4 x 5 photography is about 0.1 mm, but some people may prefer a smaller number.
You would give the focal length f in mm, and the answer would be in mm. To convert to inches divide that result by 25.4 and to convert to feet divide that result by 12.
The one third into the scene rule has never made much sense to me. It is supposed to be the point at which the rear depth of field is twice the front depth of field. It is not hard to see that this only occurs when you focus approximately at one third the hyperfocal distance. But when you focus at that distance, you can be sure the depth of field won't extend to infinity. The best I can tell is that it is a rule which might make sense when you want a scene mostly in the middle distance and you don't want to think about it too much.
The rule which most of us use requires little calculation. Focus first on the furthest point you want in focus, mark the position on the rail, then focus at the nearest point you want in focus and mark that position on the rail. Measure the distance, called the focus spread, between those points in mm and then focus at the point on the rail halfway between them. If you multiply the focus spread by 10 and divide by 2, that will give you a rough estimate of the proper f-number to use to be sure near and far points are in focus. But, as noted above, this is based on assuming a perfect lens, so it is prudent to stop down half to a full stop beyond that. This may work well as long as you don't have to stop down too far. If you end up stopping down to f/32 or beyond, diffraction may enter. In that case, you want to try to balance the effect of defocus against that diffraction. Pau l Hansma has developed a rule for doing this. It is described along with other approaches at the LF website at
/www.largeformatphotography.info/fstop.html
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