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Grassmann Algebra

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TheInteriorProduct.nb 19<br />

Y � ToScalarProducts�X�<br />

1 � ax� c �e1 � e3� �e2 � e2� � c �e1 � e2� �e2 � e3� �<br />

b �w � z� x � y � b �w � y� x � z � b �w � x� y � z<br />

ToMetricForm�Y�<br />

1 � ax� c �1,3 �2,2 � c �1,2 �2,3 �<br />

b �w � z� x � y � b �w � y� x � z � b �w � x� y � z<br />

Inner products of basis elements<br />

The inner product of two basis m-elements has been expressed in various forms previously.<br />

Here we collect together the results for reference. Here, gij is the metric tensor, g is its<br />

determinant, and Α and Β refer to any basis elements.<br />

m m<br />

ei<br />

m<br />

ei<br />

m<br />

e i<br />

m<br />

Α m ���� Β m<br />

� Β m<br />

���� ej m �∆ j<br />

i<br />

���� ej<br />

m<br />

���� ej<br />

m<br />

� ei<br />

m<br />

� ei<br />

m<br />

���� Α �<br />

����� ���� ����<br />

Α ���� Βm � Βm ����<br />

�����<br />

Αm<br />

m m<br />

e i<br />

m<br />

���� ej<br />

m<br />

�����<br />

����<br />

����� i<br />

ej � g�e ���� ej<br />

m ����� m ����� m<br />

�∆ j i<br />

� gm<br />

ij<br />

����� �����<br />

j 1<br />

���� e � ���� ei ���� ej � g<br />

m g ����� m<br />

����� m<br />

mij<br />

6.6 The Measure of an m-element<br />

The definition of measure<br />

The measure of an element Α m is denoted �Α m � and defined as the positive square root of the<br />

inner product of Α m with itself.<br />

2001 4 5<br />

�Α m � � ������������<br />

Α m ���� Α m<br />

6.37<br />

6.38<br />

6.39<br />

6.40<br />

6.41

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