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Grassmann Algebra

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TheInteriorProduct.nb 40<br />

� ����� �<br />

Since the proof of formula 6.103 is valid for any simple Α it is also valid for Αm (which is equal<br />

m<br />

to<br />

�����<br />

Α<br />

m<br />

� ) since this is also simple. The proof of formula 6.104 is then completed by applying<br />

formula 6.107.<br />

The next three sections will look at some applications of these formulae.<br />

6.11 Angle<br />

Defining the angle between elements<br />

The angle between 1-elements<br />

The interior product enables us to define, as is standard practice, the angle between two 1elements<br />

Cos�Θ� 2 � �x1<br />

� ���� x2<br />

� � 2<br />

Diagram of two vectors showing the angle between them.<br />

However, putting Α m equal to x1 and x equal to x2 in formula 6.101 yields:<br />

�x1<br />

� � x2<br />

� � 2 � �x1<br />

� ���� x2<br />

� � 2 � 1<br />

This, together with the definition for angle above implies that:<br />

Sin�Θ� 2 � �x1<br />

� � x2<br />

� � 2<br />

This is a formula equivalent to the three-dimensional cross product formulation:<br />

Sin�Θ� 2 � �x1<br />

� � x2<br />

� � 2<br />

but one which is not restricted to three-dimensional space.<br />

Thus formula 6.110 is an identity equivalent to sin 2 �Θ� � cos 2 �Θ� � 1.<br />

The angle between a 1-element and a simple m-element<br />

6.110<br />

6.111<br />

6.112<br />

One may however carry this concept further, and show that it is meaningful to talk about the<br />

angle between a 1-element x and a simple m-element Α for which the general formula [6.102]<br />

m<br />

holds.<br />

2001 4 5

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