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Grassmann Algebra

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TheInteriorProduct.nb 32<br />

�Α m � Β k<br />

x p � x1<br />

r<br />

Interior Product Formula 7<br />

p<br />

� ���� x � � ���1�<br />

p r�0<br />

rm Ν<br />

���<br />

i�1<br />

�<br />

�<br />

� x1 � x2 � x2 � � � xΝ<br />

p�r r p�r<br />

r<br />

���Α ���� xi<br />

m p�r<br />

����<br />

��Β<br />

� k<br />

���� xi�<br />

r<br />

� xΝ , Ν��<br />

p�r<br />

p<br />

r �<br />

In formula 6.72 putting Β equal to Α expresses a simple p-element in terms of products with a<br />

k<br />

m<br />

unit m-element.<br />

x p � x1<br />

r<br />

p<br />

x � � ���1�<br />

p r�0<br />

r��n�m� Ν<br />

���<br />

i�1<br />

� ���Α<br />

� �<br />

� xi<br />

���<br />

�<br />

���� �Α ���� xi�<br />

�m<br />

p�r�<br />

m r<br />

� x1 � x2 � x2 � � � xΝ<br />

p�r r p�r<br />

r<br />

6.9 The Cross Product<br />

Defining a generalized cross product<br />

� xΝ , Ν��<br />

p�r<br />

p<br />

r �<br />

The cross or vector product of the three-dimensional vector calculus of Gibbs et al. [Gibbs<br />

1928] corresponds to two operations in <strong>Grassmann</strong>'s more general calculus. Taking the crossproduct<br />

of two vectors in three dimensions corresponds to taking the complement of their<br />

exterior product. However, whilst the usual cross product formulation is valid only for vectors<br />

in three dimensions, the exterior product formulation is valid for elements of any grade in any<br />

number of dimensions. Therefore the opportunity exists to generalize the concept.<br />

Because our generalization reduces to the usual definition under the usual circumstances, we<br />

take the liberty of continuing to refer to the generalized cross product as, simply, the cross<br />

product.<br />

The cross product of Α m and Β k<br />

is denoted Α �Β and is defined as the complement of their<br />

m k<br />

exterior product. The cross product of an m-element and a k-element is thus an (nÐ(m+k))element.<br />

Α m �Β k<br />

���������<br />

�Α�Β m k<br />

6.74<br />

This definition preserves the basic property of the cross product: that the cross product of two<br />

elements is an element orthogonal to both, and reduces to the usual notion for vectors in a three<br />

dimensional metric vector space.<br />

2001 4 5<br />

6.75<br />

6.76

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