A crystal is a 3D solid bounded by flat surfaces. These geometric components are the basic "parts" of a crystal.
This is simply another term for an apex or vertex. It is the "corner" formed by the intersection of three or more faces, enclosing a three-dimensional angle.
This is one of the most fundamental measurements in crystallography.
Interfacial Angle: The angle between the perpendicular lines (called "normals") drawn to two adjacent crystal faces.
Important: It is not the internal or external angle between the faces themselves. This measurement is taken using an instrument called a goniometer. The constancy of this angle is the basis for the first law of crystallography.
A Zone is a group or set of crystal faces whose intersection edges are all mutually parallel.
Steno's Law (1669): All crystals of the same substance have constant interfacial angles between their corresponding faces.
This means a tiny, perfectly-formed quartz crystal and a large, distorted quartz crystal will have the exact same angle between their corresponding faces. This law proves that the external shape is a reflection of a fixed, ordered internal structure.
Haüy's Law (1784): The intercepts that any crystal face makes with the crystallographic axes can be expressed as simple whole-number ratios of the unit intercepts.
This law established the concept of a unit cell—a fundamental repeating block. It means faces are not random; they must align with planes of atoms in the lattice. This law is the basis for the Miller Indices system.
These are notation systems used to describe the orientation of a crystal face relative to the crystallographic axes (imaginary lines labeled a, b, and c).
An older, clunky system. It describes a face by its direct intercepts on the axes, relative to a "unit face."
The use of infinity (∞) makes this system difficult for calculations.
The modern, standard notation. It solves the "infinity problem" by using reciprocals.
How to find the Miller Indices (hkl):
All crystals are classified into 7 systems based on the lengths of their crystallographic axes (a, b, c) and the angles between them (α, β, γ).
This classification is based on symmetry. The main symmetry elements are:
The "Normal Class" (or Holohedral Class) is the class within each system that has the highest possible symmetry.
| System | Axial Relations | Angular Relations | Symmetry of Normal Class (H-M Symbol) | Example |
|---|---|---|---|---|
| Cubic | a = b = c | α = β = γ = 90° | Many axes (3 A₄, 4 A₃, 6 A₂) and 9 mirror planes (m 3̄ m) | Pyrite, Garnet |
| Tetragonal | a = b ≠ c | α = β = γ = 90° | One 4-fold axis, 4 A₂, 5 mirror planes (4/m 2/m 2/m) | Zircon, Rutile |
| Orthorhombic | a ≠ b ≠ c | α = β = γ = 90° | Three 2-fold axes, 3 mirror planes (2/m 2/m 2/m) | Barite, Topaz |
| Hexagonal | a₁ = a₂ = a₃ ≠ c | γ = 120°, α = β = 90° | One 6-fold axis, 6 A₂, 7 mirror planes (6/m 2/m 2/m) | Beryl, Apatite |
| Trigonal (Rhombohedral) | a₁ = a₂ = a₃ ≠ c | γ = 120°, α = β = 90° | One 3-fold axis, 3 A₂, 3 mirror planes (3̄ 2/m) | Calcite, Quartz |
| Monoclinic | a ≠ b ≠ c | α = γ = 90°, β > 90° | One 2-fold axis, 1 mirror plane (2/m) | Gypsum, Orthoclase |
| Triclinic | a ≠ b ≠ c | α ≠ β ≠ γ ≠ 90° | Only a center of symmetry (ī) (or nothing) | Albite, Kyanite |