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Grassmann Algebra

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Glossary.nb 2<br />

Dimension of a <strong>Grassmann</strong> algebra<br />

The dimension of a <strong>Grassmann</strong> algebra is the sum of the dimensions of its component<br />

exterior linear spaces.<br />

The dimension of a <strong>Grassmann</strong> algebra is then given by 2n , where n is the dimension of the<br />

underlying linear space.<br />

Direction<br />

A direction is the space of a vector and is therefore the set of all vectors parallel to a given<br />

vector.<br />

Displacement<br />

A displacement is a physical interpretation of a vector. It may also be viewed as the<br />

difference of two points.<br />

Exterior linear space<br />

An exterior linear space of grade m, denoted �, is the linear space generated by m-elements.<br />

m<br />

Force<br />

A force is a physical entity represented by a bound vector. This differs from common usage<br />

in which a force is represented by a vector. For reasons discussed in the text, common use<br />

does not provide a satisfactory model.<br />

Force vector<br />

A force vector is the vector of the bound vector representing the force.<br />

General geometrically interpreted 2-element<br />

A general geometrically interpreted 2-element U is the sum of a bound vector P�x and a<br />

bivector W. That is, U � P�x + W.<br />

Geometric entities<br />

Points, lines, planes, … are geometric entities. Each is defined as the space of a<br />

geometrically interpreted element.<br />

A point is a geometric 1-entity.<br />

A line is a geometric 2-entity.<br />

A plane is a geometric 3-entity.<br />

Geometric interpretations<br />

Points, weighted points, vectors, bound vectors, bivectors, … are geometric interpretations<br />

of m-elements.<br />

Geometrically interpreted algebra<br />

A geometrically interpreted algebra is a <strong>Grassmann</strong> algebra with a geometrically<br />

interpreted underlying linear space.<br />

2001 4 26

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