• Pixel-art sticker of Braggette, personifying Bragg's Law, with the caption “Planes In Step, Bright Spot.”

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Braggette

Bragg's Law Physics

\[2d\sin\theta = n\lambda\]
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Meet Braggette, for whom planes in step make a bright spot: X-rays reflecting off stacked atomic planes add up brightly only when the extra path, 2d sin θ, is a whole number of wavelengths. William Henry and William Lawrence Bragg used this in 1913 to measure crystal structures. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

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Flat $6 shipping on every order, worldwide, whatever's in it.

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Returns & replacements21 days

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The physics

Meet Braggette, an X-ray who only shines back brightly from a crystal at just the right angle.

A crystal is a regular stack of atomic planes a distance d apart. X-rays reflecting from neighbouring planes travel different distances, with the deeper ray going an extra 2d sin θ. When that extra path is a whole number n of wavelengths, the reflected waves line up and add into a strong beam. At other angles they largely cancel. This is Bragg's law, 2d sin θ = nλ.

William Henry Bragg and his son William Lawrence Bragg worked this out in 1913 and used it to work out crystal structures. They shared the 1915 Nobel Prize in Physics. Example: copper Kα X-rays (λ ≈ 0.154 nm) reflecting from planes 0.2 nm apart give a first-order peak at sin θ ≈ 0.385, θ ≈ 23°.

X-ray diffraction revealed the structure of salt, metals and minerals, and of biological molecules: Rosalind Franklin's X-ray images were key evidence for the double helix of DNA. It is still a standard tool in materials science and drug research.

Real crystals have defects and thermal motion, which broaden and weaken the peaks.

Equations

\[2d\sin\theta = n\lambda\]
Symbols
SymbolMeaningUnit
\(d\) spacing between atomic planes \(\mathrm{m}\)
\(\theta\) glancing angle between the ray and the planes \(\mathrm{rad}\)
\(n\) order of the reflection (1, 2, 3, …) —
\(\lambda\) X-ray wavelength \(\mathrm{m}\)