Pythagorean Theorem: Relationships in Euclidean Space

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Discussion Overview

The discussion centers on the application of the Pythagorean theorem in higher dimensions, particularly in relation to the lengths and volumes of linear solids such as parallelograms and parallelepipeds. Participants explore the implications of projecting these shapes onto orthonormal bases and the mathematical relationships that arise from such projections.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the Pythagorean theorem can be generalized to higher dimensions, suggesting that the length of a vector can be related to its projections onto an orthonormal basis.
  • Others argue that the focus should be on lengths rather than volumes when discussing these projections, emphasizing that the relationship is about length squared rather than volume.
  • A participant references a paper discussing the calculation of k-volumes in n-space, indicating that determinants are a key tool in this context.
  • Another participant presents a specific case involving orthonormal vectors in R^4, suggesting that the sum of the squares of projection coefficients equals one.
  • One participant provides a detailed mathematical explanation involving the wedge product and inner products to show how the area of a parallelepiped can be derived from its projections onto basis vectors.
  • There is a repeated emphasis on the distinction between length and volume in the context of these discussions, with some participants seeking clarification on the implications of their claims.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of the Pythagorean theorem to higher dimensions, with some supporting the generalization while others maintain that the focus should remain on lengths rather than volumes. The discussion remains unresolved with multiple competing views present.

Contextual Notes

Some participants express uncertainty about the definitions and implications of their claims, particularly regarding the relationship between projections and the dimensions involved. There are also references to specific mathematical formulas that have not been fully resolved or proven within the discussion.

lavinia
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The Pythagorean theorem relates the length of a vector to its projection onto an orthonormal basis for Euclidean space.

Does it also work in the same way for parallograms, and higher dimensional linear solids such as paralleopipeds? I take an n dimensional linear solid and project it onto an orthonormal basis for the space of n dimensional solids and then compute its hypervolume from the sum of squares of the projection coefficients.
 
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Here is a nice paper on this

http://www.jyi.org/volumes/volume2/issue1/articles/barth.html"

Basically the determinant is the general tool for calculation of a k-volume in k-space, but this paper explains doing k-volume in n-space when k<n.
 
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I really don't know what you mean.

in higher dimensions
Length^2 = a^2 + b^2 + c^2 + d^2...length not volume[/color]
 
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granpa said:
I really don't know what you mean.

in higher dimensions
Length^2 = a^2 + b^2 + c^2 + d^2...length not volume[/color]

If i have an orthonormal basis for a vector space then I can project linear solids onto elementary linear solids formed from the basis vectors. The projection coefficients are related to the volume of the original solid by some formula. The formula generalizes the Pythagorean theorem - and must logically be a consequence of it.
 
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I just gave you the higher dimensional generalization of the Pythagorean theorem.

its length not volume.
 
perhaps you can explain what you mean using a square as an example

[URL]http://202.38.126.65/navigate/math/history/Diagrams/PythagorasTheorem.gif[/URL]
 
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BruceG said:
Here is a nice paper on this

http://www.jyi.org/volumes/volume2/issue1/articles/barth.html"

Basically the determinant is the general tool for calculation of a k-volume in k-space, but this paper explains doing k-volume in n-space when k<n.

Thanks for this paper. It was helpful. It does not deal with the problem of projections onto an orthonormal basis for linear solids. Do you have another reference?
 
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Ok here is a special case.

take an orthonormal basis E1 ... E4 in R^4 and two orthonormal vectors

X and Y.

X and Y span a square of area 1 and can be written as linear combinations of the squares spanned by the basis E1 ... E4.

X^Y = z12 E1^E2 + ... z34E3^E4

An ugly but straight forward computation shows that sum zij^2 = 1. ( I think)
 
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Here is a simple way to show your claim is correct. Take some parallelepiped and project it onto the basis vectors:

[tex]X_1 \wedge X_2 \wedge \ldots \wedge X_p = \sum_I a_I \; e^I[/tex]

where I is some ordered multi-index, and e^I stands for the wedge product of all the e^i in I. The square of the p-volume in this parallelepiped is given by

[tex]g(X_1 \wedge X_2 \wedge \ldots \wedge X_p,X_1 \wedge X_2 \wedge \ldots \wedge X_p)[/tex]

where g is the natural extension of the inner product to the p-th exterior power of our vector space. Expanding in the orthonormal basis,

[tex]g(X_1 \wedge X_2 \wedge \ldots \wedge X_p,X_1 \wedge X_2 \wedge \ldots \wedge X_p) = \sum_I \sum_J a_I a_J \; g(e^I, e^J)[/tex]

The terms in the sum on the right vanish unless the multi-indices I and J are identical (this is because the basis is orthonormal; e.g. the projection of e1^e2^e3 on e1^e2^e4 is zero, etc.). Therefore only the diagonal part of the sum contributes, giving

[tex]\mathrm{Area}(X_1 \wedge X_2 \wedge \ldots \wedge X_p)^2 = \sum_I a_I^2[/tex]

as desired.
 
  • #10
Ben Niehoff said:
Here is a simple way to show your claim is correct. Take some parallelepiped and project it onto the basis vectors:

[tex]X_1 \wedge X_2 \wedge \ldots \wedge X_p = \sum_I a_I \; e^I[/tex]

where I is some ordered multi-index, and e^I stands for the wedge product of all the e^i in I. The square of the p-volume in this parallelepiped is given by

[tex]g(X_1 \wedge X_2 \wedge \ldots \wedge X_p,X_1 \wedge X_2 \wedge \ldots \wedge X_p)[/tex]

where g is the natural extension of the inner product to the p-th exterior power of our vector space. Expanding in the orthonormal basis,

[tex]g(X_1 \wedge X_2 \wedge \ldots \wedge X_p,X_1 \wedge X_2 \wedge \ldots \wedge X_p) = \sum_I \sum_J a_I a_J \; g(e^I, e^J)[/tex]

The terms in the sum on the right vanish unless the multi-indices I and J are identical (this is because the basis is orthonormal; e.g. the projection of e1^e2^e3 on e1^e2^e4 is zero, etc.). Therefore only the diagonal part of the sum contributes, giving

[tex]\mathrm{Area}(X_1 \wedge X_2 \wedge \ldots \wedge X_p)^2 = \sum_I a_I^2[/tex]

as desired.

thanks. That's very cool. I guess I was trying to prove this formula for the square of the p-volume. Will keep trying. It makes it a lot easier knowing that it is true.
 
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