MINERALS AND SYNTHETIC COMPOUNDS, ABmXn, W/ CLOSE PACKED X ATOMS,

AND A ATOMS OCCUPY TETRAHEDRAL AND B ATOMS OCTAHEDRAL INTERSTICES

 
.

Cu2AlMn

                  click here to see a key to this data bar                                  

tetra/octa

100%

fcc

3-d

all faces

Al- 6c/fcc; Cu- 4c, Mn - 6c

.

  structure

.
. .
     In the crystal structure of Cu2AlMn the aluminum atoms are arranged FCC, the .
copper atoms occupy 100% of the tetrahedral voids, and the manganese atoms .
occupy 100% of the octahedral voids.  The constituent atoms have relatively small
differences in their volumes and electro negativities with non-directional metallic
bonding.  Since their radius ratios are nearly equal to one, the crystal structure is
topologically equivalent to an expanded FCC lattice similar to diamond previously.
That is, the large "interstitial atoms" expand the FCC arrayed aluminum atoms so
that they do not contact each other, only the copper or manganese atoms they are
coordinated around.
  .
Ex. Cu2AlMn   ( Cu - A , Mn - B ; Al - X ) .
.
Crystal lattice
     Since all the atoms are approximately the same size the lattice model for the FCC
elements shown previously can represent the crystal structure.  It is understood that
the tetrahedra and octahedra represent the AX4 and BX6 coordinated groups of atoms
respectively.
.
Polyhedral framework

 

Cu2AlMn.gif

 

linking surfaces

   Figure 106 -  Cu2AlMn polyhedral
                 framework model

all faces

         

 

                     click image to enlarge
.      
     The polyhedral framework model pictured here emphasizes that the crystal is
built up from the packing together of the AX4 and BX6 coordination groups of atoms.
It is simply a space filling of tetrahedra and octahedra.  The formula reflects the 2:1
ratio of tetrahedra to octahedra in the packing and hence there is twice as many
copper atoms as manganese atoms.
.

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