Archived posting to the Leica Users Group, 2001/08/03
[Author Prev] [Author Next] [Thread Prev] [Thread Next] [Author Index] [Topic Index] [Home] [Search]D Khong stirred the pot with: >If I am not mistaken, pin-hole lenses are used in architectural >photography. Straight lines must be strait, everything is in focus, the >image is distortion free. Dan, I wonder if you are referring to glass lenses with a very very small aperture rather than a plain pinhole (hence the term 'pinhole lens')? Despite what someone or other claims, a plain pinhole does not focus light rays (LUGgers please contact me off-list if you disagree with that statement) so the image they produce always looks rather blurred. The addition of a simple refractive (eg glass) element to a pinhole that is not diffraction limited improves the image significantly because it brings the light rays to a focus. The aberrations created by the refractive element will be small because of the very small aperture. This is a really easy experiment to carry out if you have a close-up lens. So-called 'Pinhole Lenses' are frequently used in surveillance video cameras and the like. These are generally a bit of a misnomer, because they are small refractive lenses (often glass in the better ones) of very short focal length and wider aperture than a plain pinhole. Typical specs might be an f/2 4mm lens or an f/1 2.8 mm lens. They can have focussing mounts - which a plain pinhole would not need because it doesn't focus. For distortion-free images with a pinhole the film should be held on an arc with the pinhole at the origin (strictly speaking the film should be held on a spherical surface - beginning to look a bit like an eye). The diffraction-limited resolution is dependent upon the 'focal length' of the pinhole. The formula for diffraction limiting can be easily re-written to give the pinhole diameter in terms of the 'focal length': d^2 = 2 * wavelength * focal length This gives the following lengths (in mm), pinhole sizes (in mm), f stops and resolutions (in lppmm) using the wavelength of red light: 28 0.20 f/141 2.5 (eg a Leica body cap with a hole in it) 35 0.22 f/158 2.3 50 0.26 f/189 1.9 75 0.32 f/231 1.5 100 0.37 f/267 1.3 150 0.46 f/327 1.1 Regards, Malcolm