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Grassmann Algebra

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ExploringClifford<strong>Algebra</strong>.nb 28<br />

� Α, Β, and Γ<br />

m k p<br />

����Γ<br />

�p<br />

† ���� Γp<br />

are totally orthogonal<br />

����Α<br />

�<br />

� ��� �<br />

�m<br />

p�<br />

�<br />

�<br />

���à p<br />

�<br />

� ��� �<br />

k�<br />

������Α<br />

� Β� Αi ���� Βj �Αi���� Γs �Βj���� Γs � 0<br />

� m k<br />

Calculating with Clifford products<br />

12.45<br />

The previous section summarizes some alternative formulations for a Clifford product when its<br />

factors contain a common element, and when they have an orthogonality relationship between<br />

them. In this section we discuss how these relations can make it easy to calculate with these type<br />

of Clifford products.<br />

� The Clifford product of totally orthogonal elements reduces to the<br />

exterior product<br />

If we know that all the factors of a Clifford product are totally orthogonal, then we can<br />

interchange the Clifford product and the exterior product at will. Hence, for totally orthogonal<br />

elements, the Clifford and exterior products are associative, and we do not need to include<br />

parentheses.<br />

Α m �Β k<br />

�Γ p<br />

�Α m �Β k<br />

� Γ �Α� Β �Γ�Α�Β � Γ<br />

p m k p m k p<br />

Αi ���� Βj �Αi ���� Γs �Βj ���� Γs � 0<br />

12.46<br />

Note carefully however, that this associativity does not extend to the factors of the m-, k-, or pelements<br />

unless the factors of the m-, k-, or p-element concerned are mutually orthogonal. In<br />

which case we could for example then write:<br />

Example<br />

Α1 �Α2 � � �Αm �<br />

Α1 � Α2 � � � Αm Αi ���� Αj � 0 i � j<br />

12.47<br />

For example if x�y and z are totally orthogonal, that is x����z � 0 and y����z � 0, then we can write<br />

2001 4 26<br />

�x � y� � z � x � y � z � x ��y � z� ��y ��x � z�

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