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Grassmann Algebra

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TheInteriorProduct.nb 38<br />

Or, more succinctly:<br />

�<br />

�Α � x<br />

� 2 �<br />

� � �Α ���� x<br />

� 2<br />

�<br />

m<br />

m<br />

Similarly, formula 6.98 reduces to a more obvious decomposition for x in terms of a unit melement.<br />

� 1<br />

� � m�1 � �<br />

x � �Α � x� ���� Αm � ��1� �Αm ���� �Αm ���� x�<br />

m<br />

6.102<br />

6.103<br />

Because of its geometric significance when Α is simple, the properties of this equation are worth<br />

m<br />

investigating further. It will be shown that the square (scalar product with itself) of each of its<br />

terms is the corresponding term of formula 6.100. That is:<br />

� � � � � �<br />

��Α � x� ���� Αm � ���� ��Αm � x� ���� Αm � � �Αm � x� ���� �Αm � x�<br />

m<br />

� � � � � �<br />

�Α ���� �Αm ���� x�� ���� �Αm ���� �Αm ���� x�� � �Αm ���� x� ���� �Αm ���� x�<br />

m<br />

Further, by taking the scalar product of formula 6.102 with itself, and using formulae 6.100,<br />

6.103, and 6.104, yields the result that the terms on the right-hand side of formula 6.102 are<br />

orthogonal.<br />

� � � �<br />

��Α � x� ���� Αm � ���� �Αm ���� �Αm ���� x�� � 0<br />

m<br />

It is these facts that suggest the name triangle formulae for formulae 6.101 and 6.102.<br />

Diagram of a vector x decomposed into components in and orthogonal to Α m .<br />

The measure of the triangle components<br />

�<br />

Let Α �Α1� � � Αm , then:<br />

m<br />

� � � � m � � � �<br />

��Α � x� ���� Αm � ���� ��Αm � x� ���� Αm � � ��1� ���Αm � x� ���� ��Αm � x� ���� Αm �� ���� Αm<br />

m<br />

Focussing now on the first factor of the inner product on the right-hand side we get:<br />

2001 4 5<br />

� � � � �<br />

�Α � x� ���� ��Αm � x� ���� Αm � � �Α1 � � � Αm � x� ���� ��Α � x� ���� Αm �<br />

m<br />

m<br />

6.104<br />

6.105<br />

6.106

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