Archived posting to the Leica Users Group, 1998/05/02
[Author Prev] [Author Next] [Thread Prev] [Thread Next] [Author Index] [Topic Index] [Home] [Search]Hello Jeff, You stated: "Now, I've always heard that depth-of-field is a function of focal "length, distance and aperture -- optical formula isn't supposed to enter "into it -- and while at some level this has to be just a convenient "approximation, since there are optical formulas which are demonstrably "more sharp than others, what I've seen seems more dramatic than I'd "expect given the widespread acceptance of the depth-of-field `rules'. "BUT: there's a potential explanation. I also noticed that the "diaphragm-shaped highlights produced by specular reflections in "out-of-focus areas seemed larger in diameter at the same nominal f-stop "with the ASPH than with the pre-ASPH. If the ASPH formula happened to "transmit light less efficiently than the pre-ASPH, and if the marked "`f-stops' of the lenses were calibrated to transmittance rather than "physical aperture size (this would, after all, be the choice with the "most utility given that people will wish to use external light meters "and non-TTL flashes and such), then the two lenses could have different "physical apertures at identical marked apertures, and would have the "depth-of-field characteristics appropriate to their respective physical "apertures. As you correctly note: it are convenient 'rules'. Indeed the optical formula enters into the overall equation, but that is a difficult matter. I have to remark that the path of the light rays through the ASPH is totally different from the ones in the non-ASPH version. The optical correction is also quite different. Your explanation is quite ingenious, and almost correct. The real diameter of the physical aperture can change between two lenses of identical focal length. But the amount of light passing through the lens is the same. The differences in diameter then are not caused by more or less inefficient transmission. It is the relative position of the aperture within the lenssystem that causes the differences in the physical diameter. But they behave as identical apertures. The sharpness difference you note has a different explanation. For a point A on the filmplane to be sharper than a point B the size of the light patch must be smaller. To be smaller the rays must converge more sharply. But that also means that for more distant object points behind the ones that are sharply focused the rays will meet in front of the image plane at a sharper angle and will then produce a disc of light in the image plane that is wider than in the less sharp case. It is difficult to imagine. I will try a picture next time. But the bigger shape of the unsharpness blur (or patch of light in the image plane) in the case of the ASPH gives the more pronounced unsharpness idea. It is a matter of the greater sharpness of the in focus object points of the ASPH. Erwin