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Grassmann Algebra

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GeometricInterpretations.nb 32<br />

L � � ��ae�c f� bg� e1 � bf�a g� ce� e2 � cg��b e� af� e3�<br />

�a bef�g � c� e1 � e2<br />

�a ceg��b � f� e1 � e3<br />

�b cfg��e � a� e2 � e3;<br />

To verify that this line lies in both planes, we can take its exterior product with each of the<br />

planes and show the result to be zero.<br />

����1 � L, �2 � L��<br />

�0, 0�<br />

In the special case in which the planes are parallel, their intersection is no longer a line, but a<br />

bivector defining their common 2-direction.<br />

� Example: The osculating plane to a curve<br />

� The problem<br />

Show that the osculating planes at any three points to the curve defined by:<br />

P � � � ue1 � u 2 �e2 � u 3 �e3<br />

intersect at a point coplanar with these three points.<br />

� The solution<br />

The osculating plane � to the curve at the point P is given by ��P � P �<br />

� P �<br />

, where u is a scalar<br />

parametrizing the curve, and P �<br />

and P �<br />

are the first and second derivatives of P with respect to u.<br />

��P � P �<br />

� P �<br />

;<br />

P � � � ue1 � u 2 �e2 � u 3 �e3;<br />

P �<br />

P �<br />

� e1 � 2�u e2 � 3�u 2 �e3;<br />

� 2�e2 � 6�u e3;<br />

We can declare the space to be a 3-plane and the parameter u (and subscripts of it) to be a<br />

scalar, and then use <strong>Grassmann</strong>Simplify to derive the expression for the osculating plane<br />

as a function of u.<br />

�3; DeclareExtraScalars��u, u_ ��; ����<br />

2 � � e1 � e2 � 6u� � e1 � e3 � 6u 2 � � e2 � e3 � 2u 3 e1 � e2 � e3<br />

Now select any three points on the curve P1 , P2 , and P3 .<br />

2001 4 5

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