Building up a body centered cubic lattice: Difference between revisions

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{{Jmol_general|Body_centered_cubic_lattice.xyz|A body centered cubic lattice}}
* Consider:
* Consider:
# a cubic simulation box whose sides are of length <math>\left. L  \right. </math>
# a cubic simulation box whose sides are of length <math>\left. L  \right. </math>
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*<math> \alpha = \beta = \gamma = 90^0 </math>
*<math> \alpha = \beta = \gamma = 90^0 </math>
[[category: computer simulation techniques]]
[[category: computer simulation techniques]]
[[category: Contains Jmol]]

Latest revision as of 14:28, 22 July 2009


<jmol>

 <jmolApplet>
 <script>set spin X 10; spin on</script>
 <size>200</size>
 <color>lightgrey</color>
   <wikiPageContents>Body_centered_cubic_lattice.xyz</wikiPageContents>
</jmolApplet>
</jmol>
A body centered cubic lattice
  • Consider:
  1. a cubic simulation box whose sides are of length L
  2. a number of lattice positions, M given by M=2m3, with m being a positive integer
  • The M positions are those given by:
{xa=ia×(δl)ya=ja×(δl)za=ka×(δl)}

where the indices of a given valid site (ia,ja,ka) must fulfill:

  • ia,ja,ka must be either all odd or all even.
  • 0≤ia≤2m
  • 0≤ja≤2m
  • 0≤ka≤2m

and δl=L/(2m)

Atomic position(s) on a cubic cell[edit]

  • Number of atoms per cell: 2
  • Coordinates:

Atom 1: (x1,y1,z1)=(0,0,0)

Atom 2: (x2,y2,z2)=(l/2,l/2,l/2)


Cell dimensions:

  • a=b=c=l
  • α=β=γ=900