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Equation 6 · Part 4 · How Scientific Instruments and Metrology Actually Work

Symbol α

d  ≈  0.61 λnsin⁡αd \;\approx\; \frac{0.61\,\lambda}{n\sin\alpha}
α\alpha

What this part means

the numerical aperture of the imaging system.

Its job in the formula

α occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

Where the article explains it

where λ\lambda is the wavelength of the illuminating radiation, and nsin⁡\sinα\alpha is the numerical aperture of the imaging system.

The passage around this formula

An electron microscope is a useful worked example precisely because almost the entire modern instrument exists to correct for a limitation baked into its own optics. The achievable resolution of any imaging system with a circular aperture is bounded, in the simplest diffraction-limited approximation, by a form of the Rayleigh criterion: d  ≈  0.61 λnsin⁡αd \;\approx\; \frac{0.61\,\lambda}{n\sin\alpha}. where λ\lambda is the wavelength of the illuminating radiation, and nsin⁡\sinα\alpha is the numerical aperture of the imaging system. For visible light this caps optical microscopy at roughly 200 nanometres — far too coarse to resolve individual atoms, whose spacing in a solid is typically a few tenths of a nanometre. Electron microscopy…

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Learn the underlying idea

A variable is a named place for a value. Its letter is a local label: x can mean position in one formula and a data point in another.

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Sources cited in the article section

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