M / S EXPERIMENT SYSTEMSVIRTUAL LABORATORY 01

MYSIMULATOR / STRUCTURE OF MATTER

BRAGG / C24

Order from interference.

FINITE-PLANE DIFFRACTION
One crystal. Many waves. A measurable pattern.
01 / GONIOMETER
INCIDENT / λCRYSTAL STACKDETECTOR / 2θ
Drag to orbit · Scroll to zoom
3D schematic · lattice spacing exaggerated
Up to 16 representative planes shown
LIVE MODEL
SCATTERING ANGLE—
RELATIVE INTENSITY—
PATH DIFFERENCE—
03 / DIFFRACTION PROFILE
Relative intensity · linear scaleClick profile to set angle
SCATTERING ANGLE 2θ / DEGREES
04 / PHASE COHERENCE
—

Each segment is one plane.
The gold resultant gives
the total amplitude.

The experiment & model

2d sin θ = nλ. Waves reflected by successive planes accumulate a phase difference. At a Bragg angle they add constructively. A finite stack produces narrow peaks and side lobes.

We sum complex amplitudes from every plane: I = |Σ exp(i q zⱼ) / N|², with q = 4π sin θ / λ. Disorder adds fixed, seeded Gaussian displacements to plane positions. Wavelength and d use nanometres; intensity is normalized to the ideal coherent peak.

This is a monochromatic, one-dimensional, single-scattering teaching model. It omits atomic structure factors, absorption, instrument broadening and multiple scattering. It is not a powder diffractometer or a quantitative material identifier. Scientific reference ↗

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