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Grassmann Algebra

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TheInteriorProduct.nb 6<br />

����� ����� 1<br />

1 � a ���� ����<br />

a<br />

6.12<br />

� ���� 10: The interior product of two elements is congruent to the interior product of their<br />

complements in reverse order.<br />

The interior product of two elements is equal (apart from a possible sign) to the interior product<br />

of their complements in reverse order.<br />

Α m ���� Β k<br />

� ��1� �n�m���m�k�  k<br />

�����<br />

����<br />

�����<br />

Αm<br />

6.13<br />

If the elements are of the same grade, the interior product of two elements is equal to the interior<br />

product of their complements. (It will be shown later that, because of the symmetry of the<br />

metric tensor, the interior product of two elements of the same grade is symmetric, hence the<br />

order of the factors on either side of the equation may be reversed.)<br />

Α m ���� Β m<br />

� ���� 11: An interior product with zero is zero.<br />

�����<br />

�  ����<br />

�����<br />

Αm<br />

m<br />

Every exterior linear space has a zero element whose interior product with any other element is<br />

zero.<br />

Α m ���� 0 � 0 � 0 ���� Α m<br />

� ���� 12: The interior product is distributive over addition.<br />

The interior product is both left and right distributive over addition.<br />

Orthogonality<br />

�Α m �Β m<br />

Α m ���� �Β r<br />

� ���� à r<br />

� Α m ���� Γ r<br />

�Β���� Γ<br />

m r<br />

�Γ� � Α���� Β �Α���� Γ<br />

r m r m r<br />

Orthogonality is a concept generated by the complement operation.<br />

2001 4 5<br />

6.14<br />

6.15<br />

6.16<br />

6.17

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