wolves3012 said:
Why the inverse-square law? Simple explanation: Imagine a point source of light. The light leaves it in all directions but consider a given distance, say one metre, against two metres. The surface area that the light covers at 2 metres is diminished by 2 squared since it covers any area 2 times wider and 2 times higher, i.e 2x2=4 times (ok, this is a SIMPLE explanation, it actually relates to the surface area of a portion of a sphere).
Actually, there is another confusion for you. Someone can tell me if I'm wrong here but I seem to recall that the optical distance of a lens from the film isn't the same as the physical distance. For a 50mm lens the optical rear lens node is 50mm from the film, whatever camera and lens type. This would mean that SLR and rangefinder are identical.
The (slightly) longer light path in an SLR is side-tracking you; the light is being brought to focus on a given area (the film frame) and has been collected from a given area of the lens. If nothing else changes, then the length of the path is irrelevant (as I said before, scattering etc could make a minute difference). The light isn't diverging like a point source.
Incidentally, the inverse square law only applies to non-coherent light. Lasers produce coherent light and there is no loss of intensity with distance (ignoring scattering, which IS significant in air over large distances).
Thanks, but I wasn't questioning the inverse-square law itself, it is obvious.
I would imagine that in simple terms as the point sourse radiating light energy (like any other electro-magnetic radiation), it gets spread as spherical surface and the energy/power of these can be related to that surface area. As the raditaion travels farther away from the source, the sphare (radiation front or wave front) becomes larger in diameter thereby increasing the surface area, so that the farther away the light travels - the larger will be its sperical front area (to keep the things simple we aren't talking about athmospheric distortions of the wave front shape).
However, we shall remember that the source emmits constant power which gets spread over the spherical wave front (or something like that).
I.e. it we take a single point on top of the spherical wave front and measure radiated power of one at two distance X1 and X2 from the light source, when
X1 < X2, the point energy of X1 must be greater then that of X2 - that is to keep the source energy as a constant (which we assumed initially).
Perhaps I'm haveing troubles making clear my point, but in simple words it probably can be extrapolated to instanteous electrical power or active element (resistance for instance) or better, the power drawn by active load from the electrical source : Psource = Vout*Iout. As load gets increased (less resistance) - Iout that is drawn from the source gets larger. However, the source has been designed to supply a limited output power, so that to keep that natural law - as Iout increases, Vout of the source decreases proprotionally (we do not take into account any non-linear effects) in which way Pout (max) remains constant.
Well, I guess I got too carried away ...
🙂, perhaps this discussion gets way off the topic, if so I would be better to shut up and just listen to more photo-skilled fellows here to get back on the RF track....
I tend to agree that the dlight path distance diffeernces between SLR and RF are not significant enuogh to be "eaten up" by third stops...