Understanding Bragg's Law
Bragg's Law describes how X-rays reflect off the parallel atomic planes inside a crystal. When radiation of wavelength λ strikes a set of lattice planes spaced d apart at an angle θ, each plane reflects a small fraction of the beam. Those reflected waves interfere constructively — reinforcing rather than cancelling out — only when the extra distance travelled by the wave reflecting off the deeper plane is a whole number of wavelengths. That condition is written as:
nλ = 2d sin θ
What each symbol means
- n — the order of reflection, a positive integer (1, 2, 3…) describing how many whole wavelengths fit the path difference.
- λ — the wavelength of the incident radiation, typically X-rays, in angstroms (Å) or nanometers.
- d — the spacing between the parallel crystal lattice planes doing the reflecting, in the same length unit as λ.
- θ — the Bragg angle, measured between the incident beam and the crystal plane itself (not the surface normal).
Solving for the angle
Given λ, d, and n, the Bragg angle is found by rearranging the law: θ = arcsin(nλ / 2d). This calculator computes θ directly, along with 2θ — the angle between the incoming and outgoing beam that a diffractometer detector actually measures — and the ratio sin θ = nλ/2d used to get there.
Why there is a maximum order
Because sine can never exceed 1, a reflection can only exist while nλ/2d ≤ 1, i.e. nλ ≤ 2d. For a fixed wavelength and spacing, this puts a hard ceiling on which integer orders are physically observable — the calculator reports this as the maximum order n_max = floor(2d/λ). Push n past that ceiling and no real angle satisfies the equation; the calculator flags it as impossible rather than returning a number.
Typical X-ray wavelengths
- Cu Kα (copper): λ ≈ 1.5406 Å — the most common laboratory powder-diffraction source.
- Mo Kα (molybdenum): λ ≈ 0.7107 Å — shorter wavelength, used for small-molecule single-crystal work.
- Co Kα (cobalt): λ ≈ 1.7902 Å — favored for iron-containing samples to reduce fluorescence.
- Cr Kα (chromium): λ ≈ 2.2909 Å — used for large unit cells and residual-stress measurements.