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p.4 #21 · Diffraction Myth Dispelled | |
danmitchell wrote:
To use a goofy and over the top example, imagine some lens/aperture combination that produced diffraction blur that is "1mm across." This diffraction blur would cover 10% of the image from a 10mm wide sensor, but it would only cover 1% of the image from a 100mm wide sensor. (Yes, these sensor sizes are bogus and invented solely for this example, but the principle is the same.)
The problem with this is, if you had a 10x10mm sensor of four pixels (2x2 matrix), each 5mm in length and width, if that 1mm diffraction blur falls within one entire pixel, you wouldn't detect it at all. All of the energy from that one single light ray is picked up by a single pixel. In effect, you will have one perfectly sharp point even though the diffraction blur is 1mm. This is why pixel spacing and photosite size come into play.
The very reason we see blurring caused by diffraction is because single parallel rays of light are turned into a cone of light by diffraction whereby, when its projected onto a flat surface, perpendicular to the direction of the lightray, it forms an Airy disc. When energy from the airy disc falls within a single pixel, then that diffraction blur is not detected by the sensor and it appears perfectly sharp. However if the pixels are smaller and denser, that airy disc will distribute energy over multiple pixels. This is what we know as blur.
To take this concept further, the whole idea of depth of field simply boils down to what's considered "acceptibly sharp" since theoretically speaking, a focal plane is infinitismally thin. However, depending on the aperture setting, objects within a given distance from the focal plane can appear to be in focus since film/sensors cannot resolve the apparent out of focus blur, or at least not to a point where most people would deem it to out of focus. Why can't it resolve the out of focus blur, it's because although these light rays are no longer parallel and they diverge, when it hits the sensor, the pixels still capture most or all of the energy of each light ray thereby recording a sharp image.
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