Calculator
Example data table
| Crystal system | λ (Å) | 2θ (°) | (h k l) | Computed d (Å) | Computed lattice parameters |
|---|---|---|---|---|---|
| Cubic | 1.5406 | 44.7 | (1 1 0) | 2.0257 | a ≈ 2.8648 Å |
| Tetragonal | 1.5406 | 27.63 / 47.84 | (1 0 1) & (2 0 0) | 3.2254 / 1.9000 | a ≈ 3.8000 Å, c ≈ 6.1000 Å |
| Hexagonal | 1.5406 | 35.10 / 38.44 | (1 0 0) & (0 0 2) | 2.5548 / 2.3400 | a ≈ 2.9500 Å, c ≈ 4.6800 Å |
| Orthorhombic | 1.5406 | 17.37 / 14.27 / 11.95 | (1 0 0), (0 1 0), (0 0 1) | 5.1000 / 6.2000 / 7.4000 | a ≈ 5.1000 Å, b ≈ 6.2000 Å, c ≈ 7.4000 Å |
Formula used
How to use this calculator
- Select the crystal system that matches your material’s symmetry.
- Choose From XRD to input wavelength and 2θ peak positions.
- Enter Miller indices for each reflection; use additional reflections as required.
- Pick input and output units; the tool converts internally using Ångström.
- Press Calculate; results appear above the form.
- Use Download CSV or Download PDF to export the latest result.
- If you get an “independent reflections” error, choose different peaks/indices.
Professional notes
1) Why lattice parameters matter
Lattice parameters describe the repeating distances in a crystal and are central to phase identification, strain estimation, and quality control. Small shifts in a, b, or c can indicate compositional change, residual stress, temperature effects, or defect populations.
2) Inputs from diffraction patterns
This calculator uses peak positions (2θ), the X-ray wavelength λ, and Miller indices (h k l). From each peak, it computes interplanar spacing via Bragg’s law. When multiple peaks are supplied for non-cubic systems, the tool solves the linearized equations in 1/d².
3) Choosing reflections and Miller indices
Accurate indexing is critical. Select strong, well-separated peaks and avoid overlapping reflections. For tetragonal and hexagonal systems, include one reflection with nonzero l so the solution is sensitive to c. Orthorhombic solutions benefit from three peaks that vary in h, k, and l.
4) Cubic versus non-cubic solving
In cubic symmetry, one indexed reflection is enough because the geometry reduces to a = d√(h²+k²+l²). For tetragonal and hexagonal structures, two reflections determine a and c. Orthorhombic symmetry requires three reflections to solve a, b, and c.
5) Practical wavelength considerations
Common laboratory sources include Cu Kα (often near 1.5406 Å). If your instrument uses a different anode or monochromator setting, enter the correct λ and keep units consistent. Unit conversion is handled internally using Ångström as the working length scale.
6) Error sources and best practices
Peak position errors can arise from sample displacement, transparency, preferred orientation, and instrument zero shift. Improve reliability by calibrating with a standard, using refined peak centers, and selecting reflections at moderate θ where sinθ sensitivity is stable. If the tool reports “non-physical,” recheck indexing and peak assignments.
7) Interpreting results for materials analysis
Compare calculated parameters against reference values to verify phases. Systematic expansion or contraction may suggest alloying or thermal effects. When multiple peaks are available, cross-check that the recovered parameters predict consistent d-spacings for additional reflections.
8) Reporting and exporting for documentation
The CSV export is convenient for lab notebooks and spreadsheets, while the PDF export is suitable for quick reporting. Record the crystal system assumption, the reflections used, λ, and the final units. This ensures results remain reproducible across instruments and datasets.
FAQs
1) What does “lattice parameter” mean?
It is the set of unit-cell edge lengths that define the crystal’s repeating geometry. Depending on symmetry, you may report one parameter (a) or three (a, b, c).
2) Why do I need Miller indices?
Miller indices link a diffraction peak to a specific crystal plane family. Without correct (h k l), the geometric relationship between d-spacing and lattice parameters cannot be applied reliably.
3) Can I use this with higher-order diffraction (n > 1)?
The calculator assumes first-order diffraction. If your analysis uses higher orders, convert the peak to an equivalent first-order condition by adjusting d or using the fundamental reflection before solving.
4) What causes the “not independent enough” message?
It means the chosen reflections produce nearly the same equation set, so the solver cannot separate parameters. Pick reflections with different combinations of h, k, and l to improve independence.
5) Why does the tool show both Å and my selected unit?
Å values are displayed for transparency and easy comparison to references. The second set is converted to your chosen output unit for reporting and consistent formatting across projects.
6) How many peaks should I use for best accuracy?
Use the minimum required peaks for solving, then validate using additional indexed reflections externally. In practice, more peaks and full-pattern refinement provide better uncertainty control than single-peak estimates.
7) Does this replace Rietveld refinement?
No. It provides fast parameter estimates from selected peaks. Rietveld refinement uses the whole pattern and models instrumental and microstructural effects, giving more robust parameters and uncertainties.
Accurate lattice constants help reveal structure, phases, and defects.