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Grassmann Algebra

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Exploring<strong>Grassmann</strong><strong>Algebra</strong>.nb 17<br />

This algorithm is used in the general power function <strong>Grassmann</strong>Power described below.<br />

� Powers of <strong>Grassmann</strong> numbers with no body<br />

A further simplification in the computation of powers of <strong>Grassmann</strong> numbers arises when they<br />

have no body. Powers of numbers with no body will eventually become zero. In this section we<br />

determine formulae for the highest non-zero power of such numbers.<br />

The formula developed above for positive powers of <strong>Grassmann</strong> number still applies to the<br />

specific case of numbers without a body. If we can determine an expression for the highest nonzero<br />

power of an even number with no body, we can substitute it into the formula to obtain the<br />

required result.<br />

Let S be an even <strong>Grassmann</strong> number with no body. Express S as a sum of components Σ, where<br />

i<br />

i is the grade of the component. (Components may be a sum of several terms. Components with<br />

no underscript are 1-elements by default.)<br />

As a first example we take a general element in 3-space.<br />

S �Σ�Σ 2 �Σ 3 ;<br />

The (exterior) square of S may be obtained by expanding and simplifying S�S.<br />

��S � S�<br />

Σ � Σ 2 �Σ 2 � Σ<br />

which simplifies to:<br />

S � S � 2�Σ � Σ 2<br />

It is clear from this that because this expression is of grade three, further multiplication by S<br />

would give zero. It thus represents an expression for the highest non-zero power (the square) of<br />

a general bodyless element in 3-space.<br />

To generalize this result, we proceed as follows:<br />

1) Determine an expression for the highest non-zero power of an even <strong>Grassmann</strong> number with<br />

no body in an even-dimensional space.<br />

2) Substitute this expression into the general expression for the positive power of a <strong>Grassmann</strong><br />

number in the last section.<br />

3) Repeat these steps for the case of an odd-dimensional space.<br />

The highest non-zero power pmax of an even <strong>Grassmann</strong> number (with no body) can be seen to<br />

be that which enables the smallest term (of grade 2 and hence commutative) to be multiplied by<br />

itself the largest number of times, without the result being zero. For a space of even dimension n<br />

this is obviously pmax = n ���� 2 .<br />

For example, let X be a 2-element in a 4-space.<br />

2<br />

2001 4 5

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