Laplace Transform of Error Function: Laplace-Transform of (erfc(1/sqrt{t}))

mario99

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There are some steps that if I apply them I can show that L{erfc(t)}=1s(11s+1)\displaystyle \mathscr{L}\{\text{erfc}{(\sqrt{t})}\} = \frac{1}{s}\left(1 - \frac{1}{\sqrt{s + 1}}\right). If I apply the same steps to find L{erfc(1t)}\displaystyle \mathscr{L}\bigg\{\text{erfc}\bigg(\frac{1}{\sqrt{t}}\bigg)\bigg\}, they don't work.

How do I show the following?

L{erfc(a2t)}=eass\displaystyle \mathscr{L}\bigg\{\text{erfc}\bigg(\frac{a}{2\sqrt{t}}\bigg)\bigg\} = \dfrac{e^{-a\sqrt{s}}}{s}

Can the first identity help me to find the second identity or I have to start everything from scratch?
 
I don't immediately see a way to use the first identity. I will attempt to show by definition of Laplace transform.

L{erfc(a2t)}=0est(12π0a2tex2dx)dt=1s2π00a2testex2dxdt \displaystyle\mathcal L\left\{\operatorname{erfc}\left(\dfrac{a}{2 \sqrt t}\right)\right\} = \int_0^\infty e^{-st} \left(1 - \dfrac2{\sqrt \pi} \int_0^{\frac a{2\sqrt t}} e^{-x^2}\,dx\right)\,dt = \dfrac1s - \dfrac2{\sqrt \pi} \int_0^\infty \int_0^{\frac a{2\sqrt t}} e^{-st} e^{-x^2}\,dx\,dt
We change the order of integration of the double integral:
L{erfc(a2t)}=1s2π00a24x2estex2dtdx=1s2π01exp(a2s4x2)sex2dx \displaystyle\mathcal L\left\{\operatorname{erfc}\left(\dfrac{a}{2 \sqrt t}\right)\right\} = \dfrac1s - \dfrac2{\sqrt \pi} \int_0^\infty \int_0^{\frac{a^2}{4x^2}} e^{-st} e^{-x^2}\,dt\,dx = \dfrac1s - \dfrac2{\sqrt \pi} \int_0^\infty \dfrac{1 - \exp\left(-\dfrac{a^2s}{4x^2}\right)}s e^{-x^2}\,dx
Expand and we have
L{erfc(a2t)}=1s2sπ0ex2dx+2sπ0exp(x2a2s4x2)dx=2sπ0exp(x2a2s4x2)dx=2sπ0exp((xas2x)2as)dx \displaystyle\mathcal L\left\{\operatorname{erfc}\left(\dfrac{a}{2 \sqrt t}\right)\right\} =\dfrac1s - \dfrac2{s\sqrt \pi} \int_0^\infty e^{-x^2}\,dx + \dfrac2{s \sqrt \pi} \int_0^\infty \exp\left(-x^2 - \dfrac{a^2s}{4x^2}\right)\,dx = \dfrac2{s \sqrt \pi} \int_0^\infty \exp\left(-x^2 - \dfrac{a^2s}{4x^2}\right)\,dx = \dfrac2{s\sqrt \pi} \int_0^\infty \exp\left(-\left(x - \dfrac{|a|\sqrt s}{2x}\right)^2 - |a| \sqrt s\right)\,dx
So
L{erfc(a2t)}=2eassπ0exp((xas2x)2)dx \displaystyle \mathcal L\left\{\operatorname{erfc}\left(\dfrac{a}{2 \sqrt t}\right)\right\} = \dfrac{2e^{-|a|\sqrt s}}{s\sqrt \pi} \int_0^\infty \exp\left(-\left(x - \dfrac{|a|\sqrt s}{2x}\right)^2\right)\,dx
We are left with an integral that can be solved easily with the right trick. Use the Cauchy-Schlömilch transformation here and we get
L{erfc(a2t)}=2eassπ0exp(x2)dx \displaystyle \mathcal L\left\{\operatorname{erfc}\left(\dfrac{a}{2 \sqrt t}\right)\right\} = \dfrac{2e^{-|a|\sqrt s}}{s\sqrt \pi} \int_0^\infty \exp\left(-x^2\right)\,dx
The rest is trivial.
 
I started solving this problem in the same way you did, but did not see the idea of changing the order of integration. What a bright mind you have to spot that.

The trick that you did at the end, Cauchy-Schlömilch transformation, I have never heard of it before. The funny thing was that we tried to solve an integral a few months ago, and we got the same form of this transformation, but we were stuck to solve it. We used all the ideas we knew but failed to arrive to a solution until the thread was closed.

See the thread, post #4


Even the Great Dan, did not see this trick!😱

Thank you MaxWong. Everyday, we learn something new.
 
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