Cubic crystal system: Difference between revisions
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The simple cubic system consists of one atom on each corner. Please note that the atoms on the edges, faces, or corners of the unit cell are only partly in the cell. Thus, the simple cubic unit cell contains only one atom (1/8th * 8). Also, though in the picture, atoms are shown as dots, the atoms are really touching, filling the majority of the volume of the atom. The atomic packing factor, the fraction of space occupied by the atoms, is only .524. Due to its low density, it is a high energy structure and is rare in nature. |
The simple cubic system consists of one atom on each corner. Please note that the atoms on the edges, faces, or corners of the unit cell are only partly in the cell. Thus, the simple cubic unit cell contains only one atom (1/8th * 8). Also, though in the picture, atoms are shown as dots, the atoms are really touching, filling the majority of the volume of the atom. The atomic packing factor, the fraction of space occupied by the atoms, is only .524. Due to its low density, it is a high energy structure and is rare in nature. |
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The body centered cubic, abbreviated BCC, contains one atom in the center and the eight corner atoms. Thus, it has (1/8th *8 + 1) 2 atoms in the cell. However, due to its design, has a density of .680. Its low energy structure makes it fairly common in nature. |
The body centered cubic, abbreviated BCC, contains one atom in the center and the eight corner atoms. Thus, it has (1/8th *8 + 1) 2 atoms in the cell. However, due to its design, has a density of .680. Its low energy structure makes it fairly common in nature, including Iron, Chromium, and Tungsten. |
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Face centered cubic (FCC), contains one atom in each corner and one on each face. Thus, it has (1/8 * 8 + 1/2*6) 4 atoms in it's cell. It has a density of .741, a ratio that it shares with several other systems, including hexagonal close packed and one version of tetrahedral BCC. This number, .741, is the most tightly packed crystal possible with spherical atoms, |
Face centered cubic (FCC), contains one atom in each corner and one on each face. Thus, it has (1/8 * 8 + 1/2*6) 4 atoms in it's cell. It has a density of .741, a ratio that it shares with several other systems, including hexagonal close packed and one version of tetrahedral BCC. This number, .741, is the most tightly packed crystal possible with spherical atoms. It is extremely common, including Lead, Aluminum, Copper, and Gold. |
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=Multi-Element Compounds= |
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Several ionicaly bonded atoms also form a cubic structure. |
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[[Image:Sodium_chloride_crystal.png|thumb|left|The [[Sodium Chloride]] |
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⚫ | When the compound is formed of two elements whose ions are of roughly the same size, they have what is called the "interpenetrating simple cubic", where two atoms of a different type have individual simple cubic crystals. However, the unit cell consists of the atom of one being in the middle of the four corners, structurally resembling body centered cubic. The most common example is CsCl. |
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However, if the cation is slightly smaller than the anion (a cation/anion radius ratio of .414 to .732), it forms a different structure, "Interpenetrating FCC". When drawn separately, both atoms are arranged in an FCC structure. |
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⚫ | When the two |
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=This article is under construction= |
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The cubes drawn are the conventional unit cells. For a cube whose vertices include 000 and 200, bcc has additional [[lattice]] point 111, while fcc has 110, 101, and 011. For bcc the [[primitive cell]]s have a volume of 1/2 of the cube, e.g. the [[parallelepiped]] 000 200 020 220 111 311 131 331 with primitive translation vectors 200, 020, and 111, with determinant 4. For fcc the primitive cells have a volume of 1/4 of the cube, e.g. the parallelepiped 110 220 020 130 101 211 011 121 with primitive translation vectors 110, -1 1 0, and 0 -1 1, with determinant 2. |
The cubes drawn are the conventional unit cells. For a cube whose vertices include 000 and 200, bcc has additional [[lattice]] point 111, while fcc has 110, 101, and 011. For bcc the [[primitive cell]]s have a volume of 1/2 of the cube, e.g. the [[parallelepiped]] 000 200 020 220 111 311 131 331 with primitive translation vectors 200, 020, and 111, with determinant 4. For fcc the primitive cells have a volume of 1/4 of the cube, e.g. the parallelepiped 110 220 020 130 101 211 011 121 with primitive translation vectors 110, -1 1 0, and 0 -1 1, with determinant 2. |
Revision as of 18:27, 8 May 2006
This article may be confusing or unclear to readers. |
A cubic crystal system is a crystal where the unit cell, the unit which repeats to form the crystal, is in the shape of a cube. This is one of the most common shapes found in metallic crystals, and being the simplest, is the first to be taught to students.
The three Bravais lattices that form the cubic crystal system are:
simple cubic (sc) | body-centered cubic (bcc) | face-centered cubic (fcc) |
Cubic, face-centered |
The simple cubic system consists of one atom on each corner. Please note that the atoms on the edges, faces, or corners of the unit cell are only partly in the cell. Thus, the simple cubic unit cell contains only one atom (1/8th * 8). Also, though in the picture, atoms are shown as dots, the atoms are really touching, filling the majority of the volume of the atom. The atomic packing factor, the fraction of space occupied by the atoms, is only .524. Due to its low density, it is a high energy structure and is rare in nature.
The body centered cubic, abbreviated BCC, contains one atom in the center and the eight corner atoms. Thus, it has (1/8th *8 + 1) 2 atoms in the cell. However, due to its design, has a density of .680. Its low energy structure makes it fairly common in nature, including Iron, Chromium, and Tungsten.
Face centered cubic (FCC), contains one atom in each corner and one on each face. Thus, it has (1/8 * 8 + 1/2*6) 4 atoms in it's cell. It has a density of .741, a ratio that it shares with several other systems, including hexagonal close packed and one version of tetrahedral BCC. This number, .741, is the most tightly packed crystal possible with spherical atoms. It is extremely common, including Lead, Aluminum, Copper, and Gold.
Multi-Element Compounds
[[Image:Sodium_chloride_crystal.png|thumb|left|The Sodium Chloride When the compound is formed of two elements whose ions are of roughly the same size, they have what is called the "interpenetrating simple cubic", where two atoms of a different type have individual simple cubic crystals. However, the unit cell consists of the atom of one being in the middle of the four corners, structurally resembling body centered cubic. The most common example is CsCl.
However, if the cation is slightly smaller than the anion (a cation/anion radius ratio of .414 to .732), it forms a different structure, "Interpenetrating FCC". When drawn separately, both atoms are arranged in an FCC structure.
This article is under construction
The old article, which was deemed confusing, is below.
The cubes drawn are the conventional unit cells. For a cube whose vertices include 000 and 200, bcc has additional lattice point 111, while fcc has 110, 101, and 011. For bcc the primitive cells have a volume of 1/2 of the cube, e.g. the parallelepiped 000 200 020 220 111 311 131 331 with primitive translation vectors 200, 020, and 111, with determinant 4. For fcc the primitive cells have a volume of 1/4 of the cube, e.g. the parallelepiped 110 220 020 130 101 211 011 121 with primitive translation vectors 110, -1 1 0, and 0 -1 1, with determinant 2.
As can be seen by turning the base plane 45°, bcc and fcc only differ by a vertical scaling: in both cases the lattice points in the middle layer are above the centers of the squares of the base layer. Both scales are "special", allowing a cubic symmetry: for bcc the middle layer has a height of 1/2 of the grid size of the square grid of each layer, while for fcc the middle layer has a height of 1/2 √2 of that grid size. For other scalings both are the same, body-centered tetragonal.
Perpendicular to each body diagonal, fcc has hexagonal layers, with three positionings, which are cyclically changed. Two opposite vertices of the cube have two layers in between. See also: close-packing
The point groups that fall under this crystal system are listed below, followed by their representations in international notation and Schoenflies notation, and mineral examples.
name | international | Schoenflies | example | |
hexoctahedral | or | Oh | galena | |
gyroidal | 432 | O | petzite | |
diploidal | or | Th | pyrite | |
tetrahedral | Td | sphalerite | ||
tetartohedral | 23 | T |
There are 36 cubic space groups, of which 10 are hexoctahedral: Fd3c, Fd3m, Fm3c, Fm3m, Ia3d, Im3m, Pm3m, Pm3n, Pn3m, and Pn3n. Other terms for hexoctahedral are normal class, holohedral, ditesseral central class, galena type.
Halite structure
[[Image:Sodium_chloride_crystal.png|thumb|left|The Sodium Chloride Crystal Structure of type fcc. Each atom has six nearest neighbors, with octahedral geometry. This arrangement is known as cubic close packed (ccp).
Light blue = Na+ (Sodium ion)
Dark green = Cl− (Chlorine ion)]]
Sodium chloride forms fcc crystals. In these, the larger chloride ions are arranged in a cubic close-packing, while the smaller sodium ions fill the octahedral gaps between them. Each ion is surrounded by six of the other kind. This same basic structure is found in many other minerals, and is known as the halite structure.
The sodium ions indicated in blue show that the fcc lattice can also be represented by mid-edge and centered lattice points, without lattice points at the vertices of the cube.
See also
- Reciprocal lattice
- Atomium - building which is a model of a bcc unit cell, with vertical body diagonal.
References
- Hurlbut, Cornelius S.; Klein, Cornelis, 1985, Manual of Mineralogy, 20th ed., Wiley, ISBN 0471805807