I have colored gaffer's tape all over my gear usually for cine work, I will most likely end up using it for marking the rails on the 4x5 too. Someone ought to come up with an iPhone app that works like that online DOF calculator.
In trying to understand the limits of DOF vs Hyperfocal distance vs diffraction and center of confusion, I am wondering what the limits are in using the Scheimpflug theory in landscape photography where the closest object in my frame is typically about 5-7 feet with a 135mm and no closer than 4 feet with a 90mm or wider.
For example, The attached image is my very first day using 4x5. I shot the scene as a lens test of my 135mm. I first tagged the peaks in focus, then tilted until I saw the rocks in the bottom 1/4 of the frame hit focus. I then re-focused to get the peaks back in and did these steps until I saw both zones come into focus. I then stopped down to F/22 and shot the exposure.
So the lake shore in the background is soft, not ideal...
Is there another way to go about this or am I simply pushing the limits of tilt and need to stop down more, which I generally try to avoid if it gets within a stop or two of minimum aperture due to diffraction.
When there is not a focal plane that is clear to identify, how do others go about estimating it? The composition that I am referring to is leaves from a yellow-poplar sapling where no leaf is existing on the same plane, even considering the entire width of one leaf, there simply is no plane to focus on. Now the task is to estimate the best focal plane. I estimated the Schiemflug principle from outside the camera and used just the slightest front tilt, the camera was pointed downward slightly, lens to subject distance was about 3 feet with a 120mm lens on the 4x5. I then used the rear standard to bring a section of one of the leaves in focus that was not the closest leaf to the lens. I wanted achieve focus while being able to use a somewhat fast-ish shutter speed, but it was impossible (for me, as this is where I struggle a lot with LF). I wound up stopping down a good bit and having to use speeds from 1-3 seconds. Does my description here reveal a glaring mistake to anyone, or what? I'll develop these sheets tonight, if it is successful, it will be due to simple stopping down. I wonder in this situation, would it be better to just leave the lens plane un-tilted and just focus the way I did and stop down, without messing with Schiemflug---this being equivalent to pointing my 35mm down at the leaves and doing the same thing.
So how do you estimate the focus plane when there is no plane to focus on---I have a feeling the answer is just practice, practice, practice, like most other things.
Thanks
Chuck
So the lake shore in the background is soft, not ideal...
All the information you will ever need and much more is here: http://www.trenholm.org/hmmerk/
I wonder in this situation, would it be better to just leave the lens plane un-tilted and just focus the way I did and stop down, without messing with Schiemflug---this being equivalent to pointing my 35mm down at the leaves and doing the same thing.
I have a feeling the answer is just practice, practice, practice, like most other things.
Thanks
Chuck
I think you may have answered your own question.
rjbuzzclick, your sig is hilarious, I think I have about a dollar in nickels spread across all my camera bags, back packs, etc...
I also understand, based on my reading of Merklinger, that as you shift your focus, the plane actually swings around what Merklinger names a "hinge" line, located below the lens, rather than "moving parallel to itself" as Bonds was quoted as saying above.
The way I understand it----racking the camera back forward or backward from the lens causes the plane of sharp focus to rotate about the hinge line, but moving the lens forward or backward will move the plane of sharp focus parallel to itself. THis seems to make sense---picture the lens parallel with the film plane, moving the lens forward or backward moves the plane of sharp focus forward or backward parallel to itself, it seems that relationship holds if the lens is tilted.
Maybe. I'm no expert. But I don't know how, mathematically, moving the front or the back standard (without changing any other movement) is any different (optically or mathematically). The one change the front standard movement incurs is the distance between the lens and the object. But the object itself is not involved (optically, mathematically) in the relationship between tilt and plane of focus. So I don't understand how one would keep the plane parallel and the other would cause rotation. But I keep reading the book, maybe one day I'll get it.
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