· 3 min read
Bayer Demosaic Conversion Versus a True Monochrome Sensor
Why removing the color filter array raises a digital sensor's resolution and sensitivity compared with desaturating a Bayer color file to grayscale.
Written in by Simon Lehmann Editor
A fixed-body camera holds the lens parallel to the film and centred on its axis, which forces two compromises. The plane of sharp focus stays parallel to the film, so a receding subject can only be held by stopping down; and tilting the whole camera to include a tall subject makes vertical lines converge. A view camera removes both constraints by letting the lens standard and the film standard move independently. Understanding those movements means understanding two geometric rules that govern where the sharp plane lands and how the image is shaped.
A view camera is built around two movable frames joined by a bellows: the front standard carrying the lens, and the rear standard carrying the ground glass and film. Each can perform the same set of movements. Rise and fall translate a standard vertically, parallel to the film plane; shift translates it horizontally in the same parallel manner. These three are linear displacements that do not change any angle between lens and film. Tilt rotates a standard about a horizontal axis, and swing rotates it about a vertical axis; these change the relative angle of the planes. The division of labour is the key to using a view camera: as a general rule, movements applied to the front standard adjust focus without altering subject shape, while movements applied to the rear standard alter apparent perspective and the convergence of parallel lines.
When the lens plane and film plane are parallel, the plane of sharp focus is also parallel to both. Tilting or swinging the lens breaks that parallelism and the focus plane swings away with it, but not arbitrarily. The Scheimpflug principle states that the subject plane, the lens plane, and the image (film) plane must all intersect along a single common line for sharp focus across that subject plane; that line is the Scheimpflug line. The relationship is geometric rather than optical, and was patented by the Austrian army captain Theodor Scheimpflug in 1904 (British patent GB 1196), who credited the earlier 1901 patent of the French engineer Jules Carpentier. In practice this is what allows a single tilt to render a receding ground plane sharp from foreground to horizon at a modest aperture, rather than relying on depth of field alone.
The Scheimpflug condition alone does not fix where the sharp plane sits, because many subject planes can satisfy it. The hinge rule supplies the missing constraint. It identifies a second line, the hinge line, lying in a plane through the front focal point of the lens and parallel to the film. The distance from the lens to that hinge line depends only on focal length and tilt angle, given by J = f / sin theta, where f is the focal length and theta the tilt angle. Once the lens is tilted, this hinge line is fixed; refocusing with the rear standard then rotates the plane of sharp focus about it like a door on a hinge, while the wedge-shaped region of acceptable focus widens with distance. A larger tilt shortens J and lowers the hinge line, so even a few degrees of tilt produces a large swing of the focus plane.
Every movement also draws on the lens’s image circle, the disc of usable image the lens projects. Coverage must exceed the film diagonal for movements to be possible at all; rise, fall, and shift slide the format across that circle, and running out of coverage produces darkening or cut-off at the edges. The available movement is therefore as much a property of the lens as of the camera.
· 3 min read
Why removing the color filter array raises a digital sensor's resolution and sensitivity compared with desaturating a Bayer color file to grayscale.
· 3 min read
How weighting red, green and blue channels in conversion reproduces the effect of physical filters, and where sensor color response sets the limits.
· 4 min read
Silver-halide grain is a clumped, developed structure; sensor noise is photon shot noise plus read noise. Why each looks distinct in a monochrome print.
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