f-stop to Aperture Area Converter
Enter an f-number and focal length to find the aperture diameter and area.
Result
How it is calculated
The f-number N is the focal length divided by the diameter of the aperture opening, so diameter = focal length ÷ N (both in mm). The area of that circle is area = π × (diameter ÷ 2)² in mm². The relative area is 1 ÷ N², which sets f/1.0 to exactly 1, so every other value is a fraction of the light-gathering area at f/1. Both the f-number and the focal length must be above zero. Relative area is shown to five decimals, diameter and area to two. Because area depends on 1/N², one full stop (a change of N by about 1.41×) halves or doubles it; for example f/2.8 to f/4 is about half the area. The diameter is the physical opening (entrance pupil), not the front-element size.
Worked example
An 85 mm lens at f/1.8. Relative area = 1 ÷ 1.8² = 1 ÷ 3.24 = 0.30864, i.e. about 31% of an f/1.0 opening. Diameter = 85 ÷ 1.8 = 47.22 mm. Area = π × (47.22 ÷ 2)² = π × 23.61² ≈ 1,751.39 mm². Stopping down to f/2.8 on the same lens would shrink the diameter to 85 ÷ 2.8 = 30.36 mm.
Common mistakes
- Leaving the focal length at a default when switching lenses. The relative area depends only on N, but the diameter and area scale with focal length, so a 50 mm and an 85 mm lens at the same f-number have different physical openings.
- Thinking f/2 has half the light of f/1. The area goes with 1/N², so f/2 gives one quarter of the f/1 area; a full stop halves it, and f/1.4 is the full stop after f/1.
- Entering a focal length in centimetres or in a 35 mm equivalent. The field expects the real focal length in millimetres, and an equivalent value gives a diameter that is too large.
- Taking the diameter as the size of the lens front glass. It is only the effective aperture opening.
About this calculator
Relative aperture area follows area ∝ 1/N², where N is the f-number, which is why each full stop (f/2.8 to f/4, for example) halves the light-gathering area. With focal length known, the physical aperture diameter is d = focal length / N, and the physical area is π × (d/2)².
Photographers and optical engineers use this to see the actual size of the lens opening behind an abstract f-number, to sanity-check a lens's maximum aperture against its stated specs, or to compare how much physical glass and light-gathering area two lenses with different focal lengths need to reach the same f-stop.
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