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Grassmann Algebra

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TheInteriorProduct.nb 43<br />

Note that this has been simplified somewhat as permitted by the symmetry of the scalar product.<br />

By putting this in its angle form we get the usual expression for the volume of a parallelepiped:<br />

ToAngleForm�V�<br />

�<br />

���Α1� 2 �Α2�2 �Α3�2 ��1 � Cos�Θ1,2�2 � Cos�Θ1,3�2 �<br />

2 Cos�Θ1,2� Cos�Θ1,3� Cos�Θ2,3� � Cos�Θ2,3� 2 ��<br />

A slight rearrangement gives the volume of the parallelepiped as:<br />

V � �Α1� �Α2� �Α3��<br />

�<br />

�1 � 2 Cos�Θ1,2� Cos�Θ1,3� Cos�Θ2,3� � Cos�Θ1,2� 2 �<br />

Cos�Θ1,3� 2 � Cos�Θ2,3� 2 �<br />

We can of course use the same approach in any number of dimensions. For example, the<br />

'volume' of a 4-dimensional parallelepiped in terms of the lengths of its sides and the angles<br />

between them is:<br />

ToAngleForm�Measure�Α1 � Α2 � Α3 � Α4��<br />

�<br />

��Α1�2 �Α2�2 �Α3�2 �Α4�2 �1 � Cos�Θ2,3�2 � Cos�Θ2,4�2 �<br />

2 Cos�Θ1,3� Cos�Θ1,4� Cos�Θ3,4� � Cos�Θ3,4�2 �<br />

2 Cos�Θ2,3� Cos�Θ2,4���Cos�Θ1,3� Cos�Θ1,4� � Cos�Θ3,4�� �<br />

2 Cos�Θ1,2� �Cos�Θ1,4� �Cos�Θ2,4� � Cos�Θ2,3� Cos�Θ3,4�� �<br />

Cos�Θ1,3� �Cos�Θ2,3� � Cos�Θ2,4� Cos�Θ3,4��� �<br />

Cos�Θ1,4�2 Sin�Θ2,3� 2 � Cos�Θ1,3�2 Sin�Θ2,4� 2 �<br />

Cos�Θ1,2�2 Sin�Θ3,4� 2 ��<br />

6.12 Projection<br />

To be completed.<br />

6.13 Interior Products of Interpreted Elements<br />

To be completed.<br />

6.14 The Closest Approach of Multiplanes<br />

To be completed.<br />

2001 4 5<br />

6.116

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