Crystal Systems and Crystal Structure

Crystal Structure

Crystal structure refers to the orderly, repeating arrangement of atoms, ions, or molecules in a crystalline material. This arrangement defines the shape, symmetry, and properties of the crystal, influencing characteristics like strength, electrical conductivity, thermal conductivity, and optical properties. Understanding crystal structures is crucial across chemistry, physics, materials science, and engineering because the arrangement of particles greatly affects the material’s overall properties.

Key Concepts of Crystal Structure

1. Unit Cell

The unit cell is the smallest repeating unit in a crystal. Acting as the "building block" of the crystal, it contains atoms or molecules in a specific, orderly pattern. Repeating this unit cell in three dimensions forms the entire crystal lattice. Key characteristics of a unit cell include:

  • Lattice parameters: the lengths of the unit cell edges (aa, bb, and cc)
  • Angles between these edges: denoted as α\alpha, β\beta, and γ\gamma
  • 2. Crystal Lattice

    The crystal lattice is a three-dimensional grid where each point represents the position of a unit cell. This lattice creates an organized pattern through space, with lattice points that indicate where atoms or ions repeat. The French crystallographer Auguste Bravais identified 14 distinct types of crystal lattices, now known as Bravais lattices. These types describe different symmetrical arrangements of unit cells.

    3. Lattice Points

    Each lattice point represents an atom or group of atoms that repeats in space, defining the crystal’s symmetry and unique structure. Lattice points form a repetitive pattern, resulting in a lattice that helps establish the crystal's internal structure.


    Crystal Systems and Crystal Structure
    Crystal Systems and Crystal Structure 

    Translational Symmetry and Lattices

    A lattice is an ordered array generated by translating a single motif across space. The smallest repeating unit within a lattice, called the unit cell, replicates in all three dimensions to form the full lattice. In crystallography, unit cell corners are designated as lattice points, and these points connect in a way that delineates the unit cell boundaries (or crystallographic axes).

    Types of Planar and Three-Dimensional Lattices

    In two-dimensional space, only five types of lattices exist:

    • Square
    • Rectangular
    • Centered rectangular
    • Parallelogram
    • Hexagonal

    In three-dimensional space, only 14 unique lattices are possible, known as Bravais lattices. These types account for different unit cell shapes and arrangements, from simple cubes to complex hexagonal structures.

    Crystal Structure
    Crystal Structure: Two isolated tetrahedra (A & B) need more positive ions for neutrality than two sharing an oxygen (C & D). B and D are simplified versions of A and C, respectively.
    On the right: Common silicate structures. Arrows indicate directions in which structure repeats indefinitely. Common mineral examples for each structure are given.

    Symmetry in Crystal Structures

    Symmetry is a central feature of crystal structures. It describes the periodic repetition of structural features, contributing to the crystal’s overall form and classification. There are two main types of symmetry:

    Translational Symmetry: Repeats a motif (basic repeating unit) across a specific length, area, or volume.

    Point Symmetry: Repeats a motif around a central point. Key point symmetry operations include:

    • Reflection: Mirror-image symmetry across a plane.
    • Rotation: Repetition of a motif after rotating it by a fixed angle.
    • Inversion: A motif’s reflection across a center point in the crystal.
    • Rotoinversion: Combines rotation and inversion for complex symmetry.

    Crystal Classes and Systems

    Different combinations of symmetry operations categorize crystals into 32 distinct crystal classes. These classes are grouped into six crystal systems (e.g., cubic, hexagonal, tetragonal), each system based on a unique symmetry characteristic.

    Crystal Forms

    A crystal form is defined by a set of faces that are geometrically equivalent and related by symmetry operations. Simple crystals may consist of only one crystal form, while complex ones may combine multiple forms. In the isometric system, 15 different crystal forms are possible, such as prisms, pyramids, and dipyramids.

    Crystal Systems and Crystal Structure

    Importance and Applications of Crystal Structures

    The internal arrangement of atoms within a crystal structure determines properties like:

    Mechanical Strength: Close-packed structures are generally strong, whereas open structures can be more brittle.

    Electrical Conductivity: Highly symmetrical and closely packed structures like metals (FCC and BCC) have high electrical conductivity due to free electron movement.

    Optical Properties: The crystal’s arrangement affects how light passes through it, impacting properties like transparency and color.

    Thermal Conductivity: Simple, close-packed structures usually conduct heat well because of efficient vibrational energy transfer.

    These properties make crystal structures essential for various applications, including material design, pharmaceuticals, electronics, and mineralogy.

     
    Crystal Systems and Crystal Structure
    Crystal Systems and Crystal Structure 

    Crystal Systems

    Crystal systems are a way of classifying crystals based on the symmetry of their unit cells. The unit cell is the smallest repeating unit of a crystal structure.

    Every crystal class is a member of one of the seven crystal systems. These systems include the isometric, hexagonal, Trigonal, tetragonal, orthorhombic, monoclinic, and triclinic crystal systems. 

    Every crystal class which belongs to a certain crystal system will share a characteristic symmetry element with the other members of its system. For example, all crystals of the isometric system possess four 3-fold axes of symmetry which proceed diagonally from corner to corner through the center of the cubic unit cell. In contrast, all crystals of the hexagonal division of the hexagonal system possess a single six-fold axis of rotation.

    The crystal system of a mineral species may sometimes be determined in the field by visually examining a particularly well-formed crystal of the species.

    Crystal Systems

    Isometric Crystal System

    The isometric crystal system is also known as the cubic system. The crystallographic axes used in this system are of equal length and are mutually perpendicular, occurring at right angles to one another.All crystals of the isometric system possess four 3-fold axes of symmetry, each of which proceeds diagonally from corner to corner through the center of the cubic unit cell. 
     
    Crystals of the isometric system may also demonstrate up to three separate 4-fold axes of rotational symmetry. These axes, if present, proceed from the center of each face through the origin to the center of the opposite face and correspond to the crystallographic axes. Furthermore crystals of the isometric system may possess six 2-fold axes of symmetry which extend from the center of each edge of the crystal through the origin to the center of the opposite edge. Minerals of this system may demonstrate up to nine different mirror planes.       
     
    Examples of minerals which crystallize in the isometric system are halite, magnetite, and garnet. Minerals of this system tend to produce crystals of equidimensional or equant habit.

    Hexagonal Crystal System

    The hexagonal crystal system is defined by its unique lattice structure, characterized by four crystallographic axes. Three of these axes (a₁, a₂, and a₃) are of equal length and lie in the same plane, intersecting each other at 120° angles. The fourth axis, known as the c-axis, is perpendicular to this plane and is typically of a different length, either longer or shorter than the other three. The unit cell of a hexagonal crystal is often depicted as a hexagonal prism, with the parameters "a" representing the length of the three equal axes and "c" representing the length of the perpendicular axis.

    In terms of symmetry, the hexagonal system is known for its six-fold rotational symmetry. This means that rotating the crystal by 60° (or multiples of 60°) around the c-axis will yield an identical appearance. This system also often includes multiple reflection planes, which contribute to the symmetrical and visually appealing nature of hexagonal crystals. Common examples of minerals that crystallize in the hexagonal system include quartz, which is one of the most abundant and well-known minerals, and beryl, which forms gemstones like emerald and aquamarine. 

    Minerals like quartz and beryl are well-known examples of crystals that form in the hexagonal system, often producing large, visually striking prismatic crystals.

    Trigonal Crystal System

    Trigonal Crystal System, examples, calcite
    Trigonal Crystal System: Examples, calcite

     

    The trigonal system exhibits a three-fold rotational symmetry rather than six-fold. This difference in symmetry results in distinct crystal forms, despite the shared lattice structure with the hexagonal system. In the trigonal system, the unit cell is often described as a rhombohedron, a skewed cube where all edges are of equal length, but the angles between them are not 90°. This skewed geometry is a hallmark of trigonal crystals, which can often be identified by their characteristic three-fold rotational symmetry. When rotated by 120° around the c-axis, these crystals appear identical. Minerals like calcite and tourmaline, which crystallize in the trigonal system, typically form rhombohedral or scalenohedral shapes that reflect this lower symmetry.

    The trigonal system can be considered a subset of the hexagonal system. Both systems share a similar lattice structure, but the key difference lies in the symmetry. Hexagonal crystals have six-fold rotational symmetry, while trigonal crystals have three-fold rotational symmetry.

    Minerals like calcite and tourmaline, which crystallize in the trigonal system, typically form rhombohedral or scalenohedral shapes that reflect this lower symmetry.

    Tetragonal Crystal System

    Minerals of the tetragonal crystal system are referred to three mutually perpendicular axes. The two horizontal axes are of equal length, while the vertical axis is of different length and may be either shorter or longer than the other two. 

    Minerals of this system all possess a single 4-fold symmetry axis. They may possess up to four 2-fold axes of rotation, a center of inversion, and up to five mirror planes.

    Mineral examples which crystallize in the tetragonal crystal system are zircon and cassiterite. These minerals tend to produce short crystals of prismatic habit.

    Orthorhombic Crystal System

    Minerals of the orthorhombic crystal system are referred to three mutually perpendicular axes, each of which is of a different length than the others. Crystals of this system uniformly possess three 2-fold rotation axes and/or three mirror planes.

    The holomorphic class demonstrates three 2-fold symmetry axes and three mirror planes as well as a center of inversion. Other classes may demonstrate three 2-fold axes of rotation or one 2-fold rotation axis and two mirror planes. 
     
    Mineral examples which belong to the orthorhombic system are olivine and barite. Crystals of this system tend to be of prismatic, tabular, or acicular habit.

    Monoclinic Crystal System

    Crystals of the monoclinic system are referred to three unequal axes. Two of these axes are inclined toward each other at an oblique angle; these are usually depicted vertically. The third axis is perpendicular to the other two. The two vertical axes therefore do not intersect one another at right angles, although both are perpendicular to the horizontal axis.

    Monoclinic crystals demonstrate a single 2-fold rotation axis and/or a single mirror plane. The holomorphic class possesses the single 2-fold rotation axis, a mirror plane, and a center of symmetry. Other classes display just the 2-fold rotation axis or just the mirror plane.

    Mineral examples which adhere to the monoclinic crystal system include pyroxene, amphibole, orthoclase, azurite, and malachite, among many others. The minerals of the monoclinic system tend to produce long prisms.
     
    Crystal Systems and Crystal Structure

    Triclinic Crystal System

    Crystals of the triclinic system are referred to three unequal axes, all of which intersect at oblique angles. None of the axes are perpendicular to any other axis. 
     
    Crystals of the triclinic system may be said to possess only a 1-fold symmetry axis, which is equivalent to possessing no symmetry at all. Crystals of this system possess no mirror planes. The holomorphic class demonstrates a center of inversion symmetry. 
     
    Mineral examples of the triclinic class include plagioclase and axinite; these species tend to be of tabular habit. 
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