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Grassmann Algebra

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TheComplement.nb 38<br />

ei<br />

m<br />

The complement of a basis element<br />

� g m<br />

ij �ej<br />

m<br />

The complement of a basis 1-element of the contravariant basis has already been defined by:<br />

g � �gij�<br />

����� 1<br />

ei � ���������� �gij�ej<br />

����� �����<br />

g<br />

Here g � �gij� is the determinant of the metric tensor. Taking the complement of equation<br />

5.22 and substituting for ei<br />

����� in equation 5.24 gives:<br />

The reciprocal relation to this is:<br />

e i<br />

����� 1<br />

�<br />

����������<br />

�����<br />

g<br />

ei<br />

�����<br />

����� ����� i<br />

ei � ge �����<br />

These formulae can be extended to basis elements of � m .<br />

Particular cases of these formulae are:<br />

2001 4 5<br />

����� �����<br />

ei �<br />

m<br />

e i<br />

����� 1<br />

�<br />

m<br />

����������<br />

�����<br />

g<br />

g �e i<br />

m<br />

�����<br />

�ei<br />

m<br />

�����<br />

1<br />

���������� �e1 �����<br />

� e2 � � � en � 1<br />

g<br />

����� � �����<br />

ge1�e2 � � � en ���������������������������� �����<br />

e1 � e2 � � � en � g<br />

5.49<br />

5.50<br />

5.51<br />

5.52<br />

5.53<br />

5.54<br />

5.55<br />

5.56

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