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Grassmann Algebra

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TheInteriorProduct.nb 7<br />

If x is a 1-element and Α is a simple m-element, then x and Α may be said to be linearly<br />

m m<br />

dependent if and only if Α � x � 0, that is, x is contained in (the space of) Α. m m<br />

Similarly, x and Α are said to be orthogonal if and only if<br />

�����<br />

Α � x � 0, that is, x is contained in<br />

m m<br />

�����<br />

Α .<br />

m<br />

By taking the complement of<br />

�����<br />

Α � x � 0, we can see that<br />

�����<br />

Αm � x � 0 if and only if<br />

m<br />

Α � x<br />

m ����� � 0. Thus it may also be said that a 1-element x is orthogonal to a simple element Α if<br />

m<br />

and only if their interior product is zero, that is, Α ���� x � 0.<br />

m<br />

If x � x1 � x2 � � � xk then Α and x are said to be totally orthogonal if and only if<br />

k m k<br />

Α ���� xi � 0 for all xi contained in x. m k<br />

However, for Α m ���� �x1 � x2 � � � xk� to be zero it is only necessary that one of the xi be<br />

orthogonal to Α m . To show this, suppose it to be (without loss of generality) x1 . Then by<br />

formula 6.5 we can write Α ���� �x1 � x2 � � � xk� as �Α ���� x1� ���� �x2 � � � xk�, whence it<br />

m m<br />

becomes immediately clear that if Α ���� x1 is zero then so is the whole product Α ���� x. m m k<br />

Just as the vanishing of the exterior product of two simple elements Α and x implies only that<br />

m k<br />

they have some 1-element in common, so the vanishing of their interior product implies only<br />

�����<br />

that Α and xk (m ³ k) have some 1-element in common, and conversely. That is, there is a 1-<br />

m<br />

element x such that the following implications hold.<br />

Α m � x k � 0 � �Α m � x � 0, x k � x � 0�<br />

Α ���� x � 0 � �<br />

�����<br />

Α � x � 0, xk � x � 0�<br />

m k m<br />

Α m ���� x k � 0 � �Α m ���� x � 0, x k � x � 0�<br />

Α ���� x � 0 � Α���� x � 0 �<br />

�����<br />

Α � x � 0 xk�x�0 m k m m<br />

� The interior product of a vector with a simple bivector<br />

Suppose x is a vector and Α � Β is a simple bivector. The interior product of the bivector Α � Β<br />

with the vector x is the vector Ξ.<br />

Ξ��Α � Β� ���� x;<br />

To explore interior products, we can use the <strong>Grassmann</strong><strong>Algebra</strong> function<br />

ToScalarProducts. Applying ToScalarProducts to expand Ξ in terms of Α and Β<br />

gives:<br />

2001 4 5<br />

6.18

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