1.7: Applications to Laplace transforms
- Page ID
- 17328
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)The Laplace transform of a function \(f\) locally integrable on \([0,\infty)\) is
\[F(s)=\int_{0}^{\infty}e^{-sx}f(x)\,dx\]
for all \(s\) such that integral converges. Laplace transforms are widely applied in mathematics, particularly in solving differential equations.
We leave it to you to prove the following theorem (Exercise [exer:26]).
[theorem:12] Suppose \(f\) is locally integrable on \([0,\infty)\) and \(|f(x)|\le M e^{s_{0}x}\) for sufficiently large \(x\). Then the Laplace transform of \(F\) converges uniformly on \([s_{1},\infty)\) if \(s_{1}>s_{0}\).
[theorem:13] If \(f\) is continuous on \([0,\infty)\) and \(H(x)=\int_{0}^{\infty}e^{-s_{0}u}f(u)\,du\) is bounded on \([0,\infty),\) then the Laplace transform of \(f\) converges uniformly on \([s_{1},\infty)\) if \(s_{1}>s_{0}.\)
If \(0\le r\le r_{1}\),
\[\int_{r}^{r_{1}}e^{-sx}f(x)\,dx =\int_{r}^{r_{1}}e^{-(s-s_{0})x}e^{-s_{0}x}f(x)\,dt =\int_{r}^{r_{1}}e^{-(s-s_{0})t}H'(x)\,dt.\]
Integration by parts yields
\[\int_{r}^{r_{1}}e^{-sx}f(x)\,dt=e^{-(s-s_{0})x}H(x)\biggr|_{r}^{r_{1}} +(s-s_{0})\int_{r}^{r_{1}}e^{-(s-s_{0})x} H(x)\,dx.\]
Therefore, if \(|H(x)|\le M\), then
\[\begin{aligned} \left|\int_{r}^{r_{1}}e^{-sx}f(x)\,dx\right|&\le& M\left|e^{-(s-s_{0})r_{1}} +e^{-(s-s_{0})r} +(s-s_{0})\int_{r}^{r_{1}}e^{-(s-s_{0})x}\,dx\right|\\ &\le &3Me^{-(s-s_{0})r}\le 3Me^{-(s_{1}-s_{0})r},\quad s\ge s_{1}.\end{aligned}\]
Now Theorem [theorem:4] implies that \(F(s)\) converges uniformly on \([s_{1},\infty)\).
The following theorem draws a considerably stonger conclusion from the same assumptions.
[theorem:14] If \(f\) is continuous on \([0,\infty)\) and
\[H(x)=\int_{0}^{x}e^{-s_{0}u}f(u)\,du\]
is bounded on \([0,\infty),\) then the Laplace transform of \(f\) is infinitely differentiable on \((s_{0},\infty),\) with
\[\label{eq:30} F^{(n)}(s)=(-1)^{n}\int_{0}^{\infty} e^{-sx} x^{n}f(x)\,dx;\]
that is, the \(n\)-th derivative of the Laplace transform of \(f(x)\) is the Laplace transform of \((-1)^{n}x^{n}f(x)\).
First we will show that the integrals
\[I_{n}(s)=\int_{0}^{\infty}e^{-sx}x^{n}f(x)\,dx,\quad n=0,1,2, \dots\]
all converge uniformly on \([s_{1},\infty)\) if \(s_{1}>s_{0}\). If \(0<r<r_{1}\), then
\[\int_{r}^{r_{1}}e^{-sx}x^{n}f(x)\,dx= \int_{r}^{r_{1}}e^{-(s-s_{0})x}e^{-s_{0}x}x^{n}f(x)\,dx =\int_{r}^{r_{1}}e^{-(s-s_{0})x}x^{n}H'(x)\,dx.\]
Integrating by parts yields
\[\begin{aligned} \int_{r}^{r_{1}}e^{-sx}x^{n}f(x)\,dx &=&r_{1}^{n}e^{-(s-s_{0})r_{1}}H(r)-r^{n}e^{-(s-s_{0})r}H(r)\\ &&-\int_{r}^{r_{1}}H(x)\left(e^{-(s-s_{0})x}x^{n}\right)'\,dx,\end{aligned}\]
where \('\) indicates differentiation with respect to \(x\). Therefore, if \(|H(x)|\le M\le \infty\) on \([0,\infty)\), then
\[\left|\int_{r}^{r_{1}}e^{-sx}x^{n}f(x)\,dx\right|\le M\left(e^{-(s-s_{0})r}r^{n}+e^{-(s-s_{0})r}r^{n} +\int_{r}^{\infty}|(e^{-(s-s_{0})x})x^{n})'|\,dx\right).\]
Therefore, since \(e^{-(s-s_{0})r}r^{n}\) decreases monotonically on \((n,\infty)\) if \(s>s_{0}\) (check!),
\[\left|\int_{r}^{r_{1}}e^{-sx}x^{n}f(x)\,dx\right|<3Me^{-(s-s_{0})r}r^{n},\quad n<r<r_{1},\]
so Theorem [theorem:4] implies that \(I_{n}(s)\) converges uniformly \([s_{1},\infty)\) if \(s_{1}>s_{0}\). Now Theorem [theorem:11] implies that \(F_{n+1}=-F_{n}'\), and an easy induction proof yields [eq:30] (Exercise [exer:25]).
[example:13] Here we apply Theorem [theorem:12] with \(f(x)=\cos ax\) (\(a\ne0\)) and \(s_{0}=0\). Since
\[\int_{0}^{x}\cos au\,du=\frac{\sin ax}{a}\]
is bounded on \((0,\infty)\), Theorem [theorem:12] implies that
\[F(s)=\int_{0}^{\infty}e^{-sx}\cos ax\,dx\]
converges and
\[\label{eq:31} F^{(n)}(s)=(-1)^{n}\int_{0}^{\infty}e^{-sx}x^{n}\cos ax\,dx, \quad s>0.\]
(Note that this is also true if \(a=0\).) Elementary integration yields
\[F(s)=\frac{s}{s^{2}+a^{2}}.\]
Hence, from [eq:31],
\[\int_{0}^{\infty}e^{-sx}x^{n}\cos ax=(-1)^{n}\frac{d^n}{ds^n} \frac{s}{s^{2}+a^{2}}, \quad n=0,1, \dots.\]