Definition:Laplace Transform/Graphical Interpretation
Definition
Define $\gamma$ as the integrand of $\ds \int_0^{\to +\infty} e^{-s t} \map f t \rd t$ as a function of $\map f t$, $s$, and $t$:
- $\map \gamma {\map f t, t; s} = \map f t \, e^{-s t}$
For any particular function $f$, holding $s$ fixed, the integrand of the Laplace Transform $\kappa$ can be interpreted as a contour.
That is, for a given function $f$ and a particular complex number $s_0$ held constant:
- $\map \kappa t: \R_{\ge 0} \to \C$
- $\map \kappa t = \map \gamma {\map f t, t; s_0}$
is a parameterization of a contour.
Examples
The following are three examples of the contours defined by the integrand defining the Laplace transform of $\map \cos t$.
Laplace Transform of $\cos t$ of $3 - 9 i$
For $\map {\laptrans {\map \cos t} } {3 - 9 i}$, notice how the contour spirals towards the origin.
Intuitively, the integral converges because as $t$ increases without bound, the contour "shrinks" as it continues its path into the origin.
Laplace Transform of $\cos t$ of $\dfrac 1 2 + 4 i$
For $\map {\laptrans {\map \cos t} } {\dfrac 1 2 + 4 i}$, though the contour is not simple, it still "shrinks" as the parameter $t$ increases without bound:
Laplace Transform of $\cos t$ of $-3 + 12 i$
From Laplace Transform of Cosine, $\map {\laptrans {\map \cos t} } {-3 + 12 i}$ does not exist.
Notice how the contour spirals outward as $t$ increases without bound, never settling at a "stable point":
Sources
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- 2003: Anders Vretblad: Fourier Analysis and its Applications: $\S 3.1$
- 2004: James Ward Brown and Ruel V. Churchill: Complex Variables and Applications (7th ed.): $\S 7.81$
- 2009: William E. Boyce and Richard C. DiPrima: Elementary Differential Equations and Boundary Value Problems (9th ed.): $\S 6.1$