- published: 17 Dec 2014
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In crystallography, the terms crystal system, crystal family, and lattice system each refer to one of several classes of space groups, lattices, point groups, or crystals. Informally, two crystals tend to be in the same crystal system if they have similar symmetries, though there are many exceptions to this.
Crystal systems, crystal families, and lattice systems are similar but slightly different, and there is widespread confusion between them: in particular the trigonal crystal system is often confused with the rhombohedral lattice system, and the term "crystal system" is sometimes used to mean "lattice system" or "crystal family".
Space groups and crystals are divided into 7 crystal systems according to their point groups, and into 7 lattice systems according to their Bravais lattices. Five of the crystal systems are essentially the same as five of the lattice systems, but the hexagonal and trigonal crystal systems differ from the hexagonal and rhombohedral lattice systems. The six crystal families are formed by combining the hexagonal and trigonal crystal systems into one hexagonal family, in order to eliminate this confusion.
In mineralogy and crystallography, a crystal structure is a unique arrangement of atoms, ions or molecules in a crystalline liquid or solid. It describes a highly ordered structure, occurring due to the intrinsic nature of its constituents to form symmetric patterns.
The box can be thought of as an array of 'small boxes' infinitely repeating in all three spatial directions. Such a unit cell is the smallest unit of volume that contains all of the structural and symmetry information to build-up the macroscopic structure of the lattice by translation.
Patterns are located upon the points of a lattice, which is an array of points repeating periodically in three dimensions. The lengths of the edges of a unit cell and the angles between them are called the lattice parameters. The symmetry properties of the crystal are embodied in its space group.
A crystal's structure and symmetry play a role in determining many of its physical properties, such as cleavage, electronic band structure, and optical transparency.
A crystal or crystalline solid is a solid material whose constituents, such as atoms, molecules or ions, are arranged in a highly ordered microscopic structure, forming a crystal lattice that extends in all directions. In addition, macroscopic single crystals are usually identifiable by their geometrical shape, consisting of flat faces with specific, characteristic orientations.
The scientific study of crystals and crystal formation is known as crystallography. The process of crystal formation via mechanisms of crystal growth is called crystallization or solidification. The word crystal is derived from the Ancient Greek word κρύσταλλος (krustallos), meaning both “ice” and “rock crystal”, from κρύος (kruos), "icy cold, frost".
Examples of large crystals include snowflakes, diamonds, and table salt. Most inorganic solids are not crystals but polycrystals, i.e. many microscopic crystals fused together into a single solid. Examples of polycrystals include most metals, rocks, ceramics, and ice. A third category of solids is amorphous solids, where the atoms have no periodic structure whatsoever. Examples of amorphous solids include glass, wax, and many plastics.
Easy tips to learn table of crystal systems
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Unit 1.8 of the course The Fascination of Crystals and Symmetry A unit cell is characterized in the first instance by its so-called metric. These are the six lattice parameters: The length of the edges, a, b, and c and the angles between these edges or faces: alpha defines the angle between edge b and c, beta is the angle between a and c, and finally gamma is the angle between a and b. Furthermore, the unit cell contains all symmetry elements of the crystal. All the crystals of the world can be classified into not more than 7 crystal systems. Regarding the metric of the unit cells there are only 7 different unit cells, in principle! - triclinic - monoclinic - orthorhombic - tetragonal, - trigonal - hexagonal - and finally cubic However, the the classification according to crystal ...
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Part one of a two-part sequence on the structure of solids.
A review of some of the important crystal structures in metals: face-centered cubic FCC (or cubic close packed CCP), body centered cubic BCC, and hexagonal close packed HCP structures. Interstitial sites are identified and explained. Close-packed planes and directions are also identified and the relationships between them discussed.
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This video is a representation of a monoclinic crystal structure in its primitive form, introducing the concept of dislocation and the effects of it in the crystal structure A monoclinic crystal structure is characterized by the fact that all of its sides are different in length, two of the angles are rectangles and one is different. monoclinic crystal structures can be primitive or End - centered ( also called ( base -centered) The firt one having one atom and the last one having two atoms in total for each crystall unit. Here we represent with clay and sticks the monoclinic crystal structure in its primitive form. For this videos as mentioned before we are going to introduce the concept of disllocation, which stands in a crystall structure context for the brak or removal of an atom or at...
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In this video MS. Dr. aastha pareek, Biyani Groups of colleges, Jaipur, explains the seven crystal system like triclinic , rhombhohedral, monoclinic etc.in which explain the symmetry of molecules, bravais space lattice and their types, and bond angles also. www.gurukpo.com, www.biyanicolleges.org
Cubic unit cells are unit cells with equal lengths of all sides and all right angles between them.
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Solid crystals are nice to look at. They occur in many different colors and have very nice geometric features - long edges, smooth faces and well defined angles. It's interesting, and perhaps not surprising, that these features result from the certain (hidden) structural patterns on the molecular and atomic scale. These patterns that occur in the structure of particles are actually made up of small repeating sections, called unit cells. In this lecture, we take a look at a representative pattern called the cubic arrangement. In particular, we look at the 3 different types of cubic unit cells (simple cubic, body-centered cubic and face-centered cubic. We demonstrate how certain atomic-scale details of the unit cell (e.g. how particle arrangement and edge length in terms of the atomic ...
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Properties of Cubic Crystals: Simple Cubic, Face-centered Cubic, Body-centered Cubic, Diamond Cubic; Crystal Coordinate Systems, Miller Indices View the complete course at: http://ocw.mit.edu/3-091F04 License: Creative Commons BY-NC-SA More information at http://ocw.mit.edu/terms More courses at http://ocw.mit.edu
Complete set of Video Lessons and Notes available only at http://www.studyyaar.com/index.php/module/81-crystal-structure Direction Indices in Lattice, Typical Examples on Direction Indices, Equivalent Directions in a Lattice, Equivalent Directions in Cubic Lattice http://www.studyyaar.com/index.php/module-video/287-crystal-directions
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Materials Science & Engineering Ceramic Crystal Structure 3.3 Timeline ----------------------------------------------------------------------------------- Ceramic Crystal System ( 01:46 - 12:45) -Minimum 2 Types of Atoms -Bonding Ionic, Covalent or Mixed -Ionic System Cation and Anion -Characteristics affecting Crystal Structure -Electrically Neutral -Cation/Anion Size Ratio Maximum Number of Opposite Charged ion Surround -Co-Ordination number depends on --------------------------------------------------------------------------------------- Video By EdupediaWorld Click Here For Playlist https://www..com/playlist?list=PLJumA3phskPFPkGEkQe6YWZs8Z1-9xkkg All Right Reserved.
Video for Crystal Lattice and Unit Cell including Face centred cubic, body centred cubic, end centred cubic etc by www.chemistryconcept.com
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Materials Science and Engineering | Slip System | 7.2 Slip Planes Single crystal - Slip (13:52) Polycrystal-Slip
Structure of Materials by Prof. Sandeep Sangal & Dr. Anandh Subramaniam,Department of Metallurgy and Material Science,IIT Kanpur.For more details on NPTEL visit http://nptel.ac.in
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