f-stop – we all know what that is, right? The size of the hole in the lens that lets light through. The faster the better, and the faster the more expensive. The faster it is, the easier it is to shoot in low light. An f0.95 Leica Noctilux is easily ten times more expensive than an f2.5 Leica Summarit, yet it’s only three stops faster.
That’s all. Right?
Zeiss ZF.2 2/28 Distagon. Notice how the front few elements almost disappear – that’s because they’re not reflecting anything. This despite a huge diffuse light source – it’s the mark of excellent coatings, and promises a T-stop close to the f-stop.
f-stop is the relationship between the physical aperture of the lens – the effective optical diameter, usually limited by the diaphragm – and the focal length. Specifically, focal length over physical aperture equals f-stop. So a 50mm f2.0 will have an effective physical aperture of 25mm. This affects one property, and one property only of the lens: the minimum depth of field. All f1.4 lenses of a given focal length will have the same depth of field. However, they may appear to have different depths of field because the speed of transition between in focus and out of focus differs depending on the optical formula of the lens. As does the quality of the bokeh. (See my other article ‘A word (or ten) on bokeh’ for more information).
T-stop (curiously, always written with a capital T) is a number measuring the effective transmission aperture of the lens – in other words, the physical aperture might be f2.0, but how well does the light actually transfer light to the image plane? Why would it even differ from the f-stop in the first place? Lenses are actually black holes: they absorb or reflect or refract light in directions other than the imaging plane. It could be due to poor coatings, or internal polished elements, or simply having many elements – at every air/glass or glass/glass interface, 100% transmission is impossible. There will always be some reflections which decrease the effective transmission factor of a lens.
Modern coatings go a very long way towards ensuring that all light entering the lens makes it to the image plane, with flare reduction and increased contrast as a bonus. However, as lens design gets more complex – take those 18-270mm super zooms for instance – the number of elements required to correct aberrations across all focal lengths covered increases, and so does the complexity of the lens design. Remember, more surfaces means less light transmission.
Practically, this means that prime lenses will generally give you a higher shutter speed for a set aperture; it might be a small difference, or a noticeable one. Your f5.6 super zooms probably have a T-stop closer to f8 or f10. Conversely, a good prime lens with few elements and excellent coatings will give a T-stop very close to the actual f-stop.
Example 1: the older Nikon 85/1.4 D has a T stop closer to T-2; the Zeiss ZF 85/1.4 Planar yields almost double the shutter speed for the same exposure, with all other variables constant. The T-stop is around T1.47.
Example 2: ignoring the minor difference in focal length, consider the Nikon 105/2.8 VR macro and the Leica 90/4 Elmarit-M macro. The Leica has only four elements. The Nikon, 14 elements in 12 groups. What do you think their T stops are? Unsurprisingly, not very different.
Not all lenses are made equal. And don’t think because there are fewer elements, the lens design isn’t as good. It’s very difficult to design a well-corrected lens with few elements – designs such as the Cooke Triplet and Double Gauss are pretty much as simple as they get. MT
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