Laplace Transform of a Square Wave Function

Laplace Transform of a Square Wave Function
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What is the right way to find the Laplace transform of this function:

The thing I noticed was:

$$f(t)=\text{A}\space\space\space\space\space\space\space\space\space\space 0\le t<\frac{\text{T}}{2}\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space\space f(t)=-\text{A}\space\space\space\space\space\space\space\space\space\space \frac{\text{T}}{2}<t<\text{T}$$

But how do find the complete Laplace transform of this function?

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2 Answers

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We can write the square wave function as $$ f(t)=A\sum_{k=0}^{\infty} \left[u\left(t-kT\right)-2u\left(t-\frac{2k+1}{2}T\right)+u\left(t-(k+1)T\right)\right] $$ where $u(t)$ is the Heaviside's function. So the Laplace transform of $f(t)$ is \begin{align} F(s)&=A\sum_{k=0}^{\infty} \frac{1}{s}\left[\mathrm e^{-kTs}-2\mathrm e^{-\frac{2k+1}{2}Ts}+\mathrm e^{-(k+1)Ts}\right]\\ &=A\sum_{k=0}^{\infty} \frac{\mathrm e^{-kTs}}{s}\left[1-\mathrm e^{-\frac{Ts}{2}}\right]^2\\ &=\frac{A}{s}\left(1-\mathrm e^{-\frac{Ts}{2}}\right)^2\sum_{k=0}^{\infty} \mathrm e^{-kTs}\\ &=\frac{A}{s}\left(1-\mathrm e^{-\frac{Ts}{2}}\right)^2\frac{1}{1-\mathrm e^{-sT}}\\ &=\frac{A}{s}\frac{1-\mathrm e^{-\frac{Ts}{2}}}{1+\mathrm e^{-\frac{Ts}{2}}}\\ &=\frac{A}{s}\tanh\left(\frac{sT}{4}\right) \end{align}

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$\newcommand{\lap}{\mathscr{L}}\newcommand{\dd}{\mathrm{d}}$ Let us use $A=1$. Function $f$ is periodic with period $T$. In fact, it suffices to defive this function over the interval $[0, T]$ \begin{equation} f(t) = \begin{cases} 1,&\text{ for } 0 \leq t < \tfrac{T}{2} \\ -1, &\text{ for } \tfrac{T}{2} < t \leq T \end{cases}. \end{equation} As a result, the Laplace transform of $f$ exists and it is given by \begin{align*} \lap\{f\}(s) {}={}& \frac{1}{1-e^{-Ts}}\int_0^{T}e^{-s\tau}f(\tau)\dd\tau \\ {}={}& \frac{1}{1-e^{-2Ts}} \left(\int_0^{\tfrac{T}{2}}e^{-s\tau}\dd\tau - \int_{\tfrac{T}{2}}^{T}e^{-s\tau}\dd\tau \right) \\ {}={}& \frac{1}{1-e^{-2Ts}} \left( \left.-\tfrac{1}{s}e^{-s\tau}\right|_0^{\tfrac{T}{2}} {}+{} \left.\tfrac{1}{s}e^{-s\tau}\right|_{\tfrac{T}{2}}^{T} \right) \\ {}={}& \ldots \\ {}={}& \frac{1}{s}\frac{e^{\tfrac{Ts}{2}}-1}{e^{\tfrac{Ts}{2}}+1} {}={} \frac{1}{s}\tanh\left(\tfrac{Ts}{4}\right). \end{align*}

I like @alexjo's answer, but we need to use the dominated convergence theorem to guarantee that we can interchange the Laplace transform and the series.

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David Miller
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David Miller

David Miller brings 15 years of experience in global economics, personal finance strategy, and market dynamics. He specializes in turning complex economic trends into actionable insights for everyday readers.