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Grassmann Algebra

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TheExteriorProduct.nb 33<br />

xi � C1 � � � Ci�1 � C0 � Ci�1 � � � Cn<br />

�������������������������������� ��������������������������������<br />

C1 � C2 � � � Cn<br />

All the well-known properties of solutions to systems of linear equations proceed directly from<br />

the properties of the exterior products of the Ci .<br />

� Example solution<br />

Consider the following system of 3 equations in 4 unknowns.<br />

w � 2�x � 3�y � 4�z � 2<br />

2�w � 7�y � 5�z � 9<br />

w � x � y � z � 8<br />

To solve this system, first declare the unknowns w, x, y and z as scalars, and then declare a<br />

basis of dimension at least equal to the number of equations. In this example, we declare a 4space<br />

so that we can add another equation later.<br />

Next define:<br />

DeclareExtraScalars��w, x, y, z��<br />

�������<br />

2.33<br />

�a, b, c, d, e, f, g, h, w, x, y, z, �, �_ � _� ?InnerProductQ, _� 0<br />

DeclareBasis�4�<br />

�e1, e2, e3, e4�<br />

Cw � e1 � 2�e2 � e3;<br />

Cx ��2�e1 � e3;<br />

Cy � 3�e1 � 7�e2 � e3;<br />

Cz � 4�e1 � 5�e2 � e3;<br />

C0 � 2�e1 � 9�e2 � 8�e3;<br />

The system equation then becomes:<br />

wCw � xCx � yCy � zCz � C0<br />

Suppose we wish to eliminate w and z thus giving a relationship between x and y. To<br />

accomplish this we multiply the system equation through by Cw � Cz .<br />

�w Cw � xCx � yCy � zCz��Cw � Cz � C0 � Cw � Cz<br />

Or, since the terms involving w and z will obviously be eliminated by their product with<br />

Cw � Cz , we have more simply:<br />

2001 4 5<br />

�x Cx � yCy��Cw � Cz � C0 � Cw � Cz

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