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Grassmann Algebra

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TheComplement.nb 17<br />

The complement of the complement of an m-element<br />

Consider the general m-element Α ��ai�ei . By taking the complement of the complement of<br />

m m<br />

this element and substituting from equation 5.18, we obtain:<br />

����� �����<br />

Α � �<br />

m<br />

�����<br />

� �<br />

� ��1� m��n�m� �Α<br />

m<br />

i<br />

�����<br />

ai ei<br />

m<br />

i<br />

�ai���1� m��n�m� �ei<br />

m<br />

Finally then we have shown that, provided the complement mapping gij is symmetric and the<br />

constant � is such that � 2 �gij� � 1, the complement of a complement axiom is satisfied by<br />

an otherwise arbitrary mapping, with sign ��1� m��n�m� .<br />

Special cases<br />

����� ����� m��n�m� Α � ��1� �Αm<br />

m<br />

The complement of the complement of a scalar is the scalar itself.<br />

����� �����<br />

a � a<br />

The complement of the complement of an n-element is the n-element itself.<br />

����� �����<br />

Α �Αn<br />

n<br />

The complement of the complement of any element in a 3-space is the element itself, since<br />

��1�m��3�m� is positive for m equal to 0, 1, 2, or 3.<br />

Alternatively, we can say that<br />

����� �����<br />

Α �Αm except when Α is of odd degree in an even-dimensional<br />

m<br />

m<br />

space.<br />

5.7 Working with Metrics<br />

� The default metric<br />

In order to calculate complements and interior products, and any products defined in terms of<br />

them (for example, Clifford and hypercomplex products), <strong>Grassmann</strong><strong>Algebra</strong> needs to know<br />

what metric has been imposed on the underlying linear space � 1 . <strong>Grassmann</strong> and all those<br />

writing in the tradition of the Ausdehnungslehre tacitly assumed a Euclidean metric; that is, one<br />

in which gij �∆ij . This metric is also the one tacitly assumed in beginning presentations of<br />

the three-dimensional vector calculus, and is most evident in the definition of the cross product<br />

as a vector normal to the factors of the product.<br />

2001 4 5<br />

5.30<br />

5.31<br />

5.32

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