This blog page can be used for a last minute revision on the topic of ' Different types of crystal structures in metal' from the material science course.
Different types of crystal structures in metal
- There are 3 types of crystal structures in metals . They are Face- centered cubic (FCC) , Body - centered cubic ( BCC ) and Hexagonal close packed ( HCP ) .
Keywords
Crystalline
- It is a material in which the atoms positioned in a repeating or a periodic array over the large atomic distances.
Crystal structure
- It is the manner in which the atoms , ions or molecules are spatially arranged .Well , there is an extremely large number of different crystal structures that comprises a long range atomic order which varies from simple structures for metals to complex ones which are being displayed by some of the ceramic and polymeric materials.
Lattice
- It is a model which a three- dimensional array of points coinciding with the atom positions.
Face- Centered Cubic ( FCC)
Face-Centered Cubic in a unit cell |
- This lattice is a cubic shape.
- There are 8 corner atoms in each unit cell and also 6 atoms on each face of the unit cell .
- The effective total number of atoms in a face-centered cubic unit cell is 4.
Body- Centered Cubic
Body-centered cubic |
- This lattice is a cubic shape.
- There are 8 corner atoms in each unit cell and 1 centre atom is each unit cell .
- The effective total number of atoms in a body-centered cubic is 2 .
Hexagonal Close- Packed Crystal Structures
- This lattice is in a hexagonal shape .
- The hexagonal plane is also known as a basal plane.
- The top and bottom basal plane consist of 6 corner atoms.
- In the mid plane , it consist of 3 atoms .
- At the centre of the upper and lower basal planes , there is one atom .
Linear Density
- It is defined where the number of atoms per unit length where the centers lies on the direction vector for a specific crystallographic structure.
LD = Number of atoms centered on direction vector
length of direction vector
Planner Density
- Planner density is the number of atoms per unit area that are centered on a crystallographic plane.
PD = Number of atoms centered on a plane
Area of plane
Area of plane
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