JumboShrimp said:
Time for the day's stupid question:
It is a known fact that all 2x teleconverters lose 2 stops of light, and all 1.4x TCs lose one stop of light. Why? What if the glass in the TC was twice as large? ... it would let in more light, therefore the light loss would be less. Now I realize this logic is somehow flawed, but I can't reason why. Anyone?
Because stops are
RELATIVE. Stops are ultimately based on a ratio, such as f/4. That 'f' stands for 'focal length', and it's a simple mathematical formula. So, it really means 'focal length divided by four'. If you have a 400mm f/4 lens, your entrance pupil (the physical aperture as viewed through the front of the lens at "infinity") is 100mm in diameter. The f-ratio is actually determined by dividing the focal length by the entrance pupil diameter, so the 'f/4' really comes from 400mm/100mm, which equals 4.
If you slap on a 2x teleconverter, you are adding on what is effectively a magnifying glass to the end of your lens. In this case, it magnifies your subject by a factor of two, which is the same as doubling your focal length. So, now you have an 800mm lens. Thing is, the lens did not get wider...it's the same diameter, which means it has the same entrance pupil. The entrance pupil of the lens, when observed from "infinity", is still 100mm. That means that your f-ratio is now 800mm/100mm, which equals 8. You've lost two stops of light (f/4 -> f/5.6 -> f/8).
I'm sure there is still the same question, though...why? First, the entrance pupil is ultimately what determines the amount of light that will produce the image circle at the sensor plane. The AREA of the opening in the diaphragm, to be specific, is what determines the amount of light. So, a 100mm entrance pupil means you have
pi(d/2)^2 area, or 7854mm^2 circular area. Attaching a TC to a lens is adding a magnifying glass to the BACK of the lens. You've already limited the amount of light, since by the time it reaches the TC, it's already passed through the aperture. A 2x TC is effectively taking the center portion of circle of light produced by the aperture, 1/4 the area or 1964mm^2, and enlarging it to the same 7854mm^2 (which is then projected by the rest of the optics in the TC to the standard image circle size for the camera, say 44mm diameter for FF; it's really a bit more complicated than that, but for casual conversation sake).
It's taking a smaller quantity of light from the center area of the image circle and spreading it out over a greater area. In other words...one quarter the quantity of light spread out over four times the area that light initially covers results in two halvings of the intensity of light at any given pixel.