Understanding the Meaning of (e1^e2)\cdote3 in Geometric Algebra

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SUMMARY

The expression (e1^e2)·e3 in geometric algebra represents the inner product of a vector with a bivector, which geometrically projects the vector onto the plane defined by the bivector, rotates it 90 degrees, and dilates it by the magnitude of the bivector. The discussion clarifies that the volume of the parallelepiped is represented by the outer product e1 ∧ e2 ∧ e3, not the inner product. The equivalence of this construction to the double cross product in 3D is highlighted, emphasizing the intuitive nature of the geometric algebra approach compared to the vector algebra method.

PREREQUISITES
  • Understanding of geometric algebra concepts, specifically bivectors and vectors.
  • Familiarity with the inner product and outer product operations in geometric algebra.
  • Knowledge of the double cross product in vector algebra.
  • Basic comprehension of 3D geometry and projections.
NEXT STEPS
  • Study the properties and applications of bivectors in geometric algebra.
  • Learn about the geometric interpretations of inner and outer products in geometric algebra.
  • Explore the relationship between geometric algebra and vector algebra, particularly the double cross product.
  • Utilize GAViewer to visualize geometric algebra concepts and operations.
USEFUL FOR

Mathematicians, physicists, and students of advanced geometry who are interested in understanding geometric algebra and its applications in 3D space.

JakeD
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What is the meaning of (e1^e2)\cdote3?

(outer product multiplied by inner product)
 
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The volume of the parallelepiped formed by those vectors.
 
Thank you.

Jake
 
No, this is just wrong! The volume of the parallelepiped would be all outer products, e_1 \wedge e_2 \wedge e_3.

(e_1 \wedge e_2) is a bivector. So you're asking: what is the inner product of a vector with a bivector? That has a clear geometrical interpretation. For a vector a and bivector B, a \cdot B does the following:

  1. Project a onto the plane defined by B
  2. Rotate 90 degrees in the "sense" of B
  3. Dilate by the magnitude of B

Note that this uses all three defining characteristics of the bivector B:
  • Attitude (basically the angle the plane makes in space)
  • Orientation (clockwise vs. counterclockwise)
  • Magnitude (i.e. area)

With the inner product used by Hestenes et al, you also have
a \cdot B = - B \cdot a
which let's you answer your question.

By the way, in 3D, your construction is equivalent to the "double cross product" (not the "vector triple product"):
<br /> (e_1 \wedge e_2) \cdot e_3 = - (e_1 \times e_2) \times e_3<br />
Note how the GA version (described above) is much more intuitive and easy to visualize -- the VA version (double cross product) will give you carpal tunnel from all those applications of the right-hand rule!
 
Thanks chogg for your details answer; I later noticed indeed that his answer is wrong.
GAViewer also demonstrates this very nicely.
 

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