Explore crystal diffraction geometry with a Bragg angle. Choose wavelength or energy, then set spacing. Instant results help plan scans and verify peaks quickly.
This calculator uses Bragg's law for diffraction from parallel lattice planes:
nλ = 2d sin(θ)
Rearranged for angle: θ = asin(nλ / (2d)). The calculator also reports 2θ, commonly used in scans.
If nλ is larger than 2d, no real angle exists.
| Case | Input | d (Angstrom) | n | θ (deg) | 2θ (deg) |
|---|---|---|---|---|---|
| 1 | λ = 1.5406 Angstrom | 2.0000 | 1 | 22.618 | 45.236 |
| 2 | Energy = 8.047 keV | 2.0000 | 1 | 22.620 | 45.240 |
| 3 | λ = 0.15406 nm | 3.1355 | 1 | 14.220 | 28.440 |
Values are illustrative and may vary slightly with rounding.
Bragg Angle Guide
The Bragg angle (θ) is the incidence angle where waves scattered by parallel crystal planes add constructively. In diffraction experiments, it links the measured geometry to a specific interplanar spacing (d), letting you identify phases and track lattice changes.
Bragg’s law uses the radiation wavelength (λ), the plane spacing (d), and an integer diffraction order (n). Most powder diffraction peaks are analyzed with n = 1 and a known λ. The calculator converts your units so the sine argument stays dimensionless.
If you enter energy, the tool computes wavelength using the common relation λ(Å) = 12.3984193 / E(keV). For example, 8.047 keV corresponds to about 1.5406 Å, close to the Cu Kα scale used in many laboratory diffractometers.
Many instruments report the scan axis as 2θ, not θ. A peak at 2θ = 45.24° implies θ = 22.62°. Reporting both values helps when comparing scan files, reference patterns, and analytical models that may use θ directly. In Bragg–Brentano setups, the sample rotates by θ while the detector tracks 2θ.
A real Bragg angle exists only when nλ ≤ 2d. If nλ exceeds 2d, the sine argument would be greater than 1 and no physical solution is possible for that plane spacing and wavelength. This often flags a unit mismatch or an incorrect d value.
With λ near 1.54 Å and d between roughly 1–5 Å, θ commonly falls between a few degrees and about 60°, yielding 2θ up to 120°. At low angles, small alignment errors can shift peaks noticeably, so consistent geometry matters.
You can validate an instrument by comparing measured 2θ peaks against known standards. If a reference material has a well-known d-spacing, compute θ (or 2θ) and check the difference. Systematic offsets often indicate zero shift or sample displacement.
For publication-quality reporting, state λ (or E), d, n, and whether the reported angle is θ or 2θ. If d is derived from indexing or refinement, include uncertainty. Small d changes map to measurable peak shifts, especially at higher angles. For small shifts, a useful approximation is Δ(2θ) ≈ −2(Δd/d)·tan(θ) in radians, highlighting why higher-angle peaks are especially strain-sensitive.
1) Why does the calculator show both θ and 2θ?
Many diffractometers scan and report 2θ, while Bragg’s law is written with θ. Showing both avoids confusion when comparing instrument readouts, reference patterns, and theoretical calculations.
2) What does “no real solution: nλ exceeds 2d” mean?
It means the required sine value would be greater than 1, so no physical Bragg angle exists for those inputs. Check units, reduce n, use a shorter wavelength, or verify the d-spacing.
3) Which d value should I use for a crystal?
Use the interplanar spacing for the plane family (hkl) that produces the reflection. In powder diffraction, d often comes from reference databases or is computed from lattice parameters and indices.
4) Can I use this for neutrons or electrons?
Yes, as long as you know the wavelength and the relevant plane spacing. The same geometric condition applies for coherent scattering; just ensure the wavelength units match the source and experiment.
5) When should I use higher diffraction orders?
Higher orders (n > 1) can occur, but many analyses treat peaks as first order with different (hkl) planes. Use higher n only when the experimental context clearly supports it.
6) Does temperature affect the Bragg angle?
Indirectly, yes. Temperature changes the lattice spacing through thermal expansion, which shifts θ and 2θ. Tracking peak movement with temperature is a common way to study phase transitions and strain.
7) How accurate is the energy-to-wavelength conversion?
The constant used is a standard hc value expressed in keV·Å. Practical accuracy is usually limited more by beam spectrum, monochromation, and instrument alignment than by the conversion constant.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.