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Crystal structure

physical science Maturity 11-13 Next article →

A crystal structure is a precise description of how particles are arranged in a solid. These particles can be atoms, ions, or molecules. In a crystalline material, these particles do not sit in a random pile. Instead, they form highly ordered, symmetric patterns. These patterns repeat along three-dimensional space. This repeating nature is what defines a crystalline substance. The way these particles line up determines the physical properties of the material.

Sodium-chloride-3D-ionic
Sodium-chloride-3D-ionic

To understand the whole structure, scientists look at the unit cell. The unit cell is the smallest repeating unit of the crystal. It contains the full symmetry of the entire structure. You can imagine it as a single building block. When you repeat this block through translation, you build the whole crystal. The geometry of a unit cell is a parallelepiped. This shape is defined by six lattice parameters. These include three edge lengths, known as a, b, and c. They also include the three angles between those edges, called alpha, beta, and gamma.

Interplanar spacing
Interplanar spacing

Inside the unit cell, particles sit at specific locations. These locations are described by fractional coordinates. These coordinates are measured along the cell edges from a reference point. Scientists only need to report a small subset of these particles. This subset is called the crystallographic asymmetric unit. This unit is chosen to occupy the smallest possible physical space. All other particles in the cell are generated by symmetry operations. These operations are collected together into a concept called the space group. There are 230 possible space groups in three-dimensional space.

Miller Indices Cubes2
Miller Indices Cubes2

Scientists use specific math to describe directions and planes within the lattice. Crystallographic directions are lines that link the nodes of the crystal. Crystallographic planes are geometric planes that also link these nodes. To name these planes, researchers use Miller indices. These are a set of three integers, h, k, and l. These indices are proportional to the inverses of where the plane hits the unit cell axes. If an index is zero, the plane does not intersect that axis. In a cubic system, these indices act like coordinates for a vector.

Cristal densite surface
Cristal densite surface

Not all planes and directions are the same. Some planes have a higher density of nodes, meaning more particles are packed there. This density changes how the crystal behaves in the real world. For example, the refractive index of a material relates to its periodic density. High-density planes also affect chemical reactivity and surface tension. These planes often influence how a crystal breaks, a process called cleavage. They also affect how crystals deform under pressure. This is called plastic deformation.

Quartz, Tibet
Quartz, Tibet

All crystals can be classified into seven different lattice systems. These systems group structures based on their symmetry. Symmetry occurs when a pattern remains unchanged after a specific operation. For example, rotating a crystal 180 degrees might result in an identical look. This is called twofold rotational symmetry. The cubic system is the most symmetric of all. It has four threefold rotational axes. These axes are oriented at 109.5 degrees from each other. In contrast, the triclinic system is the least symmetrical.

Triclinic
Triclinic

Beyond the seven systems, there are 14 distinct Bravais lattices. These lattices describe the geometric arrangement of lattice points. Every crystalline material known today fits into one of these 14 arrangements. The crystal structure is formed by placing a basis at every lattice point. The basis is a specific group of atoms. These atoms repeat indefinitely in three dimensions. Recent science has even found new families like ZIP phases. These show dualistic atomic ordering in complex intermetallic materials.

Cubic
Cubic
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🖼️ Images & Media (21)
File:Sodium-chloride-3D-ionic.png
Sodium-chloride-3D-ionic.png
File:Miller Indices Cubes2.svg
Miller Indices Cubes2.svg
File:Cristal densite surface.svg
Cristal densite surface.svg
File:Interplanar spacing.png
Interplanar spacing.png
File:Triclinic.svg
Triclinic.svg
File:Monoclinic.svg
Monoclinic.svg
File:Base-centered monoclinic.svg
Base-centered monoclinic.svg
File:Orthorhombic.svg
Orthorhombic.svg
File:Orthorhombic-base-centered.svg
Orthorhombic-base-centered.svg
File:Orthorhombic-body-centered.svg
Orthorhombic-body-centered.svg
File:Orthorhombic-face-centered.svg
Orthorhombic-face-centered.svg
File:Tetragonal.svg
Tetragonal.svg

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