Difference between revisions of "Mallard's law"
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<font color="blue">Loi de Mallard</font>(''Fr''). <Font color="black">Legge di Mallard </Font>(''It'') | <font color="blue">Loi de Mallard</font>(''Fr''). <Font color="black">Legge di Mallard </Font>(''It'') | ||
| − | The '''law of Mallard''' was introduced by Georges Friedel (''Leçons de Cristallographie'' 1926, page 436) to explain, | + | The '''law of Mallard''' was introduced by Georges Friedel (''Leçons de Cristallographie'' 1926, page 436) to explain, for reticular bases, [[twinning by pseudomerohedry]]. |
| − | The law of Mallard states that twin elements are always rational (i.e. [[direct lattice]] elements): therefore, a [[twin element|twin plane]] is a lattice plane, and a [[twin element|twin axis]] is a lattice row. These twin elements are pseudosymmetry elements for the lattice of the individual. The twin operations produce now | + | The law of Mallard states that twin elements are always rational (i.e. [[direct lattice]] elements): therefore, a [[twin element|twin plane]] is a lattice plane, and a [[twin element|twin axis]] is a lattice row. These twin elements are pseudosymmetry elements for the lattice of the individual. The twin operations produce now slightly different orientations of the lattice of the individual, which are only quasi-equivalent, and no longer equivalent, as in the case of [[twinning by merohedry]]. |
[[Category:Fundamental crystallography]] | [[Category:Fundamental crystallography]] | ||
Revision as of 10:11, 25 May 2007
Loi de Mallard(Fr). Legge di Mallard (It)
The law of Mallard was introduced by Georges Friedel (Leçons de Cristallographie 1926, page 436) to explain, for reticular bases, twinning by pseudomerohedry.
The law of Mallard states that twin elements are always rational (i.e. direct lattice elements): therefore, a twin plane is a lattice plane, and a twin axis is a lattice row. These twin elements are pseudosymmetry elements for the lattice of the individual. The twin operations produce now slightly different orientations of the lattice of the individual, which are only quasi-equivalent, and no longer equivalent, as in the case of twinning by merohedry.