Difference between revisions of "Talk:Unit cell"
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+ | ====Extra math expressions==== | ||
+ | A given real-space cubic lattice will have dimensions: | ||
+ | :<math>\left(a,b,c\right)</math> | ||
+ | Such that the position of any particular cell within the infinite lattice is: | ||
+ | :<math>\mathbf{r}_{hkl} = \left\langle ah,bk,cl\right\rangle </math> | ||
+ | Where ''h'', ''k'', and ''l'' are indices. | ||
+ | The corresponding inverse-space lattice would be: | ||
+ | :<math> | ||
+ | \mathbf{q}_{hkl} = 2\pi \left\langle \frac{h}{a} , \frac{k}{b} , \frac{l}{c} \right\rangle | ||
+ | </math> | ||
+ | :<math> | ||
+ | q_{hkl} = 2\pi \sqrt{ \left( \frac{h}{a} \right)^2 + \left( \frac{k}{b} \right)^2 + \left( \frac{l}{c} \right)^2 } | ||
+ | </math> | ||
+ | In the case where <math>a=b=c</math>: | ||
+ | :<math> | ||
+ | \begin{alignat}{2} | ||
+ | q_{hkl} & = 2\pi \sqrt{ \left( \frac{h}{a} \right)^2 + \left( \frac{k}{a} \right)^2 + \left( \frac{l}{a} \right)^2 } \\ | ||
+ | & = \frac{2\pi}{a} \sqrt{ h^2 + k^2 + l^2 } | ||
+ | \end{alignat} | ||
+ | </math> | ||
+ | |||
====TBD: Reciprocal vector components==== | ====TBD: Reciprocal vector components==== | ||
:<math> | :<math> |
Revision as of 10:24, 18 June 2014
Extra math expressions
A given real-space cubic lattice will have dimensions:
Such that the position of any particular cell within the infinite lattice is:
Where h, k, and l are indices. The corresponding inverse-space lattice would be:
In the case where :