Exponentials as eigenfunctions in LTI Systems

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SUMMARY

The discussion centers on the concept of exponentials as eigenfunctions in Linear Time-Invariant (LTI) systems, specifically focusing on the eigenvalue equation involving the integral transform H(s). The equation presented is e^{s t} = e^{s t} H(s), where H(s) is defined as H(s) = ∫_{-\infty}^\infty h(t) e^{-s t} d t. Participants assert that the integrals H(s) and ∫_{-\infty}^{\infty} h(τ) e^{-s τ} d τ are unique, leading to a singular solution for H(s). The discussion emphasizes the uniqueness of solutions in the context of eigenvalue equations.

PREREQUISITES
  • Understanding of Linear Time-Invariant (LTI) systems
  • Familiarity with eigenvalue equations and eigenfunctions
  • Knowledge of integral transforms, specifically the Laplace transform
  • Basic principles of calculus, including the fundamental theorem of calculus
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  • Study the properties of eigenfunctions in LTI systems
  • Learn about the Laplace transform and its applications in system analysis
  • Explore the uniqueness of solutions in differential equations
  • Investigate the fundamental theorem of calculus and its implications in integral equations
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Students and professionals in electrical engineering, control systems, and applied mathematics who are interested in the analysis of LTI systems and eigenfunction properties.

Tanja
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I hope I catched the correct forum.

Under http://en.wikipedia.org/wiki/LTI_system_theory
e^{s t} is an eigenvalue.
I don't really understand that the following is an eigenvalue equation:
\quad = e^{s t} \int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau
\quad = e^{s t} H(s),

where

H(s) = \int_{-\infty}^\infty h(t) e^{-s t} d t .

The integrals H(s) and \int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau should be unique, isn't it? So there is only one solution for H(s) = \int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau with one e^{s t}, isn't it?

Thanks
Tanja
 
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[itex]e^{s t}[/itex] is an eigenvalue.
I don't really understand that the following is an eigenvalue equation:
[itex]\quad = e^{s t} \int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau[/itex]
[itex]\quad = e^{s t} H(s)[/itex],

where

[itex]H(s) = \int_{-\infty}^\infty h(t) e^{-s t} d t[/itex].

The integrals H(s) and [itex]\int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau[/itex] should be unique, isn't it? So there is only one solution for [itex]H(s) = \int_{-\infty}^{\infty} h(\tau) \, e^{-s \tau} \, d \tau[/itex] with one [itex]e^{s t}[/itex], isn't it?
[itex]F(x) = \int_a^xf(t)dt[/itex] is unique by the fundamental theorem of calculus.
 
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