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Why Sine Wave is an Eigenfunction of LTI Systems


Why a Sine Wave is an Eigenfunction of an LTI System

1. What is an Eigenfunction?

A function \( x(t) \) is called an eigenfunction of a system if:

\[ \text{System}\{x(t)\} = \lambda x(t) \]

Where:

  • The output has the same shape as the input
  • It is only scaled (and possibly phase shifted)
  • \( \lambda \) is the eigenvalue

2. LTI System Description

An LTI (Linear Time-Invariant) system is completely described by its impulse response \( h(t) \).

The output is given by convolution:

\[ y(t) = x(t) * h(t) \]

\[ y(t) = \int_{-\infty}^{\infty} x(\tau) h(t-\tau) d\tau \]

3. Use a Complex Exponential Input

Consider the input:

\[ x(t) = e^{j\omega t} \]

Substitute into convolution:

\[ y(t) = \int_{-\infty}^{\infty} e^{j\omega \tau} h(t-\tau) d\tau \]

Rewrite:

\[ e^{j\omega \tau} = e^{j\omega t} e^{-j\omega (t-\tau)} \]

\[ y(t) = e^{j\omega t} \int_{-\infty}^{\infty} h(t-\tau) e^{-j\omega (t-\tau)} d\tau \]

Let \( u = t-\tau \), then:

\[ y(t) = e^{j\omega t} \int_{-\infty}^{\infty} h(u) e^{-j\omega u} du \]

The integral is the Fourier Transform of \( h(t) \):

\[ H(j\omega) \]

Therefore:

\[ y(t) = H(j\omega) e^{j\omega t} \]

4. Final Result

\[ \boxed{ \text{LTI}\{e^{j\omega t}\} = H(j\omega) e^{j\omega t} } \]

This means:

  • Input = complex exponential
  • Output = same complex exponential
  • Only multiplied by \( H(j\omega) \)

Eigenfunction: \( e^{j\omega t} \)

Eigenvalue: \( H(j\omega) \)

5. Why Sine is Also an Eigenfunction

\[ \sin(\omega t) = \frac{e^{j\omega t} - e^{-j\omega t}}{2j} \]

Because LTI systems are linear:

\[ \sin(\omega t) \rightarrow |H(j\omega)| \sin(\omega t + \angle H(j\omega)) \]

  • Frequency does not change
  • Only amplitude and phase change

6. Intuitive Explanation

  • LTI systems cannot create new frequencies
  • LTI systems cannot shift frequency
  • They only scale and phase-shift each frequency component

Since a sine wave contains only one frequency, it passes through unchanged except for gain and phase shift.

Conclusion

\[ \boxed{ \text{Complex exponentials (and hence sine waves) are eigenfunctions of all LTI systems.} } \]

Because convolution with \( h(t) \) simply multiplies them by \( H(j\omega) \).



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