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Grassmann Algebra

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TheComplement.nb 3<br />

an m-element and an (nÐm)-element is a scalar. Thus there is the opportunity of defining for<br />

each m-element a corresponding 'co-m-element' of grade nÐm such that the regressive product of<br />

these two elements gives a scalar. We will see that this scalar measures the square of the<br />

'magnitude' of the m-element or the (nÐm)-element, and corresponds to the inner product of<br />

either of them with itself. We will also see that the notion of orthogonality is defined by the<br />

correspondence between m-elements and their 'co-m-elements'. But most importantly, the<br />

definition of this inner product as a regressive product of an m-element with a 'co-m-element' is<br />

immediately generalizable to elements of arbitrary grade, thus permitting a theory of interior<br />

products to be developed which is consistent with the exterior and regressive product axioms<br />

and which, via the notion of 'co-m-element', leads to explicit and easily derived formulae<br />

between elements of arbitrary (and possibly different) grade.<br />

The foundation of the notion of measure or metric then is the notion of 'co-m-element'. In this<br />

book we use the term complement rather than 'co-m-element'. In this chapter we will develop the<br />

notion of complement in preparation for the development of the notions of interior product and<br />

orthogonality in the next chapter.<br />

The complement of an element is denoted with a horizontal bar over the element. For example<br />

�����<br />

Α, x+y and x�y are denoted Α ,<br />

���������<br />

x � y and<br />

���������<br />

x � y.<br />

m m<br />

Finally, it should be noted that the term 'complement' may be used either to refer to an operation<br />

(the operation of taking the complement of an element), or to the element itself (which is the<br />

result of the operation).<br />

Historical Note<br />

<strong>Grassmann</strong> introduced the notion of complement (ErgŠnzung) into the Ausdehnungslehre of<br />

1862 [<strong>Grassmann</strong> 1862]. He denoted the complement of an element x by preceding it with a<br />

vertical bar, viz |x. For mnemonic reasons which will become apparent later, the notation for the<br />

complement used in this book is rather the horizontal bar: x<br />

����� . In discussing the complement,<br />

<strong>Grassmann</strong> defines the product of the n basis elements (the basis n-element) to be unity. That is<br />

�e1�e2�� �en� � 1 or, in the present notation, e1 � e2 � � � en � 1. Since <strong>Grassmann</strong><br />

discussed only the Euclidean complement (equivalent to imposing a Euclidean metric<br />

gij �∆ij ), this statement in the present notation is equivalent to 1<br />

����� � 1. The introduction of<br />

such an identity, however, destroys the essential duality between � and � which requires<br />

m n�m<br />

rather the identity 1<br />

����� �����<br />

� 1. In current terminology, equating e1 � e2 � � � en to 1 is<br />

equivalent to equating n-elements (or pseudo-scalars) and scalars. All other writers in the<br />

<strong>Grassmann</strong>ian tradition (for example, Hyde, Whitehead and Forder) followed <strong>Grassmann</strong>'s<br />

approach. This enabled them to use the same notation for both the progressive and regressive<br />

products. While being an attractive approach in a Euclidean system, it is not tenable for general<br />

metric spaces. The tenets upon which the Ausdehnungslehre are based are so geometrically<br />

fundamental however, that it is readily extended to more general metrics.<br />

2001 4 5

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