What are some real-life applications of general vector spaces?

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SUMMARY

The discussion focuses on the application of general vector spaces in teaching, particularly for introductory students. It emphasizes the importance of engaging students by connecting abstract concepts to real-life scenarios, such as using displacement vectors and the riddle involving movement in a plane. The conversation highlights the significance of understanding inner product spaces and techniques like the Gram-Schmidt Process, which can be applied to various mathematical constructs, including Fourier series and polynomials. Overall, the goal is to present vector spaces as powerful tools for solving complex problems.

PREREQUISITES
  • Understanding of Euclidean space and displacement vectors
  • Familiarity with linear algebra concepts, including systems of equations
  • Knowledge of inner product spaces and their properties
  • Basic comprehension of differential equations and their solutions
NEXT STEPS
  • Explore the Gram-Schmidt Process for orthogonalization in vector spaces
  • Study the application of inner product spaces in Fourier series
  • Investigate the relationship between linear ordinary differential equations (ODEs) and linear systems
  • Learn about the properties and applications of polynomial vector spaces
USEFUL FOR

Students, educators, and mathematicians interested in teaching or learning about the practical applications of general vector spaces and their relevance in solving mathematical problems.

matqkks
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Students familiar with Euclidean space find the introduction of general vectors spaces pretty boring and abstract particularly when describing vector spaces such as set of polynomials or set of continuous functions. Is there a tangible way to introduce this? Are there examples which will have a real impact? I would like to introduce this in an engaging manner to introductory students. Are there any real life applications of general vector spaces?
 
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I try to give my students a "dynamic" definition. Basically, a vector space is an abelian Lie group. Of course I don't say that out loud but I start with arrows in Euclidean space as "displacement vectors", then a position vector is def'ed i.t.o. displacements of an origin point. Addition becomes composition of action.

I use the riddle "I walk South 1 mile, East one mile, and then North one mile and am back where I started. Where am I?" to show that we must be careful to confirm the basic properties (and hint at more general constructs).

Then when I jump to more abstract vectors we look to the actions involved in the algebra methods, e.g. solving systems of equations evokes the act of adding functions. I try to convince them that viewing appropriate abstract constructs as vectors gives them a set of "power tools" for attacking higher order problems. I show for example the connection between solving a linear ODE, solving a linear system and solving a simple Lin. eqn. Ax=b.
 
matqkks said:
Students familiar with Euclidean space find the introduction of general vectors spaces pretty boring and abstract particularly when describing vector spaces such as set of polynomials or set of continuous functions. Is there a tangible way to introduce this? Are there examples which will have a real impact? I would like to introduce this in an engaging manner to introductory students. Are there any real life applications of general vector spaces?

Are you talking about teaching inner product spaces?

If this is the case, it was mind boggling to me when I first learned that Gram-Schmidt Process and orthogonal projection can be be applied on vector spaces such as the underlying space of Fourier series, the set of polynomials, etc. Of course, understanding inner product itself is important.

I think only those who can see the big picture of how general inner product space is, can really get the excitement.

P.S.: I'm just a student.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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