| | Introduction to Clifford Algebra |
 | | As a concrete example of addition of bivectors, consider a gyroscopic precession problem, as follows: The green bivector is the initial angular momentum of the system, and the small purple bivector is torque*time. |
 | | Q behaves exactly as we would expect a bivector to behave, based on the description given in section 1.1: a patch of surface with a direction of circulation around its edge. |
 | | The sequence would have been: (a) establish a few fundamental notions; (b) set forth the behavior of the basis vectors according to equation 22 and equation 23; (c) express all vectors, bivectors, etc. in terms of their components relative to this basis; and (d) derive the main results in terms of components. |
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