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InverseLaplaceTransform ​

The inverse Laplace transform, as a small dictionary of common images (s−ns^{-n}, 1/(s−a)1/(s-a), s/(s2±a2)s/(s^2 \pm a^2), a/(s2±a2)a/(s^2 \pm a^2)) plus linearity — not a general residue calculus.

✓ checked against that system · ! checked, with disagreements (hover a chip)Wolfram LanguageInverseLaplaceTransform✓
InverseLaplaceTransform(F, s, t)f(t)f(t) such that L{f}(s)=F(s)\mathcal{L}\{f\}(s) = F(s), read off a fixed table of images.
Typed signatures
TypePackageApplies
(expression, expression, expression) -> expressionanalyticalways

Domain: Transforms

Details
  • Covered: s−ns^{-n} (nn a positive integer) →tn−1/(n−1)!\to t^{n-1}/(n-1)!; 1/(s−a)→eat1/(s-a) \to e^{at}; s/(s2+a2)→cos⁡(at)s/(s^2+a^2) \to \cos(at); a/(s2+a2)→sin⁡(at)a/(s^2+a^2) \to \sin(at); s/(s2−a2)→cosh⁡(at)s/(s^2-a^2) \to \cosh(at); a/(s2−a2)→sinh⁡(at)a/(s^2-a^2) \to \sinh(at); sums and a constant factor.
  • Also, from the usual tables (each confirmed against wolframscript): s−ν→tν−1/Γ(ν)s^{-\nu}\to t^{\nu-1}/\Gamma(\nu) for a non-whole ν>0\nu>0 and its first two ν\nu-derivatives (a factor ln⁡(cs)\ln(cs) or ln⁡2(cs)\ln^2(cs), c>0c>0); the shifting theorems (e−csF→f(t−c) θ(t−c)e^{-cs}F\to f(t-c)\,\theta(t-c), and F(s−a)→eatf(t)F(s-a)\to e^{at}f(t) when a s−a\sqrt{s-a} appears, once); 1/((s−a)s)→eaterf⁡(at)/a1/((s-a)\sqrt s)\to e^{at}\operatorname{erf}(\sqrt{at})/\sqrt a and s/(s−a)\sqrt s/(s-a); ln⁡s/(s−a)→eat(ln⁡a−Ei(−at))\ln s/(s-a)\to e^{at}(\ln a-\mathrm{Ei}(-at)) for a concrete a>0a>0; Γ(ν,s)/sν→tν−1θ(t−1)\Gamma(\nu,s)/s^\nu\to t^{\nu-1}\theta(t-1); erf⁡(as)/s→θ(a−t)/πt\operatorname{erf}(\sqrt{as})/\sqrt s\to\theta(a-t)/\sqrt{\pi t} for a>0a>0; and the elliptic pairs K(a2/s2)−π/2K(a^2/s^2)-\pi/2 and s(π/2−E(a2/s2))s(\pi/2-E(a^2/s^2)), both Bessel I0I1I_0I_1 products.
  • s−ν/2Kν(bs)→2ν−1b−νtν−1e−b2/4ts^{-\nu/2}K_\nu(b\sqrt s)\to 2^{\nu-1}b^{-\nu}t^{\nu-1}e^{-b^2/4t} for b>0b>0 and the order matching the power of ss (from L{tν−1e−a/t}=2(a/s)ν/2Kν(2as)\mathcal{L}\{t^{\nu-1}e^{-a/t}\}=2(a/s)^{\nu/2}K_\nu(2\sqrt{as})).
  • Declined: anything outside those — a general rational function of s (partial-fraction decomposition is not attempted), a non-positive power of s, a bare logarithm, an image that doesn't depend on s at all.

Examples

Basic #

L−1{1/s2}=t\mathcal{L}^{-1}\{1/s^2\} = t

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InInverseLaplaceTransform(1s2,s,t)\mathrm{InverseLaplaceTransform}(\frac{1}{s^2}, s, t)Outtt

L−1{1/(s−a)}=eat\mathcal{L}^{-1}\{1/(s-a)\} = e^{at}

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InInverseLaplaceTransform(1s−a,s,t)\mathrm{InverseLaplaceTransform}(\frac{1}{s-a}, s, t)Outexp⁡(at)\exp(at)

L−1{s/(s2+a2)}=cos⁡(at)\mathcal{L}^{-1}\{s/(s^2+a^2)\} = \cos(at)

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InInverseLaplaceTransform(ss2+a2,s,t)\mathrm{InverseLaplaceTransform}(\frac{s}{s^2+a^2}, s, t)Outcos⁡(at)\cos(at)
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InInverseLaplaceTransform(1s+1,s,t)\mathrm{InverseLaplaceTransform}(\frac{1}{s+1}, s, t)Outexp⁡(−t)\exp(-t)
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InInverseLaplaceTransform(ln⁡(a+sb+s),s,t)\mathrm{InverseLaplaceTransform}(\ln(\frac{a+s}{b+s}), s, t)Out1t(exp⁡(−(bt))−exp⁡(−(at)))\frac{1}{t}(\exp(-(bt))-\exp(-(at)))
Scope #
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InInverseLaplaceTransform(aa2+s2,s,t)\mathrm{InverseLaplaceTransform}(\frac{a}{a^2+s^2}, s, t)Outsin⁡(at)\sin(at)
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InInverseLaplaceTransform(sa2+s2,s,t)\mathrm{InverseLaplaceTransform}(\frac{s}{a^2+s^2}, s, t)Outcos⁡(at)\cos(at)
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InFullSimplify(InverseLaplaceTransform(as2−a2,s,t))\mathrm{FullSimplify}(\mathrm{InverseLaplaceTransform}(\frac{a}{s^2-a^2}, s, t))Outsinh⁡(at)\sinh(at)
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InFullSimplify(InverseLaplaceTransform(ss2−a2,s,t))\mathrm{FullSimplify}(\mathrm{InverseLaplaceTransform}(\frac{s}{s^2-a^2}, s, t))Outcosh⁡(at)\cosh(at)
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InInverseLaplaceTransform(s(a2+s2)2,s,t)\mathrm{InverseLaplaceTransform}(\frac{s}{(a^2+s^2)^2}, s, t)Outtsin⁡(at)2a\frac{t\sin(at)}{2a}
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InInverseLaplaceTransform(s(a2+s2)(b2+s2),s,t)\mathrm{InverseLaplaceTransform}(\frac{s}{(a^2+s^2)(b^2+s^2)}, s, t)Outcos⁡(at)b2−a2+cos⁡(bt)a2−b2\frac{\cos(at)}{b^2-a^2}+\frac{\cos(bt)}{a^2-b^2}
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InFullSimplify(InverseLaplaceTransform(s2(s2−a2)(s2−b2),s,t))\mathrm{FullSimplify}(\mathrm{InverseLaplaceTransform}(\frac{s^2}{(s^2-a^2)(s^2-b^2)}, s, t))Outasinh⁡(at)a2−b2+bsinh⁡(bt)b2−a2\frac{a\sinh(at)}{a^2-b^2}+\frac{b\sinh(bt)}{b^2-a^2}
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InInverseLaplaceTransform(exp⁡(−5s)(s−2)s,s,t)\mathrm{InverseLaplaceTransform}(\frac{\exp(-5s)}{(s-2)\sqrt{s}}, s, t)Out12(2erf⁡(2(t−5))HeavisideTheta(t−5)exp⁡(2(t−5)))\frac{1}{2}(\sqrt{2}\operatorname{erf}(\sqrt{2(t-5)})\mathrm{HeavisideTheta}(t-5)\exp(2(t-5)))
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InInverseLaplaceTransform(b+sa+s,s,t)\mathrm{InverseLaplaceTransform}(\frac{\sqrt{b+s}}{a+s}, s, t)Out(erf⁡(t×(b−a))exp⁡(t×(b−a))b−a+1πt)exp⁡(−(bt))(\operatorname{erf}(\sqrt{t×(b-a)})\exp(t×(b-a))\sqrt{b-a}+\frac{1}{\sqrt{π}\sqrt{t}})\exp(-(bt))
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InInverseLaplaceTransform(ln⁡(s)s−1,s,t)\mathrm{InverseLaplaceTransform}(\frac{\ln(s)}{s-1}, s, t)Out−(ExpIntegralEi(−t)et)-(\mathrm{ExpIntegralEi}(-t)e^{t})
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InInverseLaplaceTransform(ln⁡(s2+1s2+2),s,t)\mathrm{InverseLaplaceTransform}(\ln(\frac{s^2+1}{s^2+2}), s, t)Out−1t(2(cos⁡(t)−cos⁡(2t)))-\frac{1}{t}(2(\cos(t)-\cos(\sqrt{2}t)))
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InInverseLaplaceTransform(ln⁡(4s)s3,s,t)\mathrm{InverseLaplaceTransform}(\frac{\ln(4s)}{\sqrt[3]{s}}, s, t)Out−ln⁡(t)+2ln⁡(2)−3ln⁡(3)2−3π6−γΓ(13)t23\frac{-\ln(t)+2\ln(2)-\frac{3\ln(3)}{2}-\frac{\sqrt{3}π}{6}-γ}{Γ(\frac{1}{3})t^{\frac{2}{3}}}
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InInverseLaplaceTransform(ln⁡(s)2s,s,t)\mathrm{InverseLaplaceTransform}(\frac{\ln(s)^2}{s}, s, t)Out(−ln⁡(t)−γ)2−π26(-\ln(t)-γ)^2-\frac{π^2}{6}
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InInverseLaplaceTransform(Γ(13,s)s3,s,t)\mathrm{InverseLaplaceTransform}(\frac{Γ(\frac{1}{3}, s)}{\sqrt[3]{s}}, s, t)OutHeavisideTheta(t−1)t23\frac{\mathrm{HeavisideTheta}(t-1)}{t^{\frac{2}{3}}}
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InInverseLaplaceTransform(erf⁡(2s)s,s,t)\mathrm{InverseLaplaceTransform}(\frac{\operatorname{erf}(\sqrt{2s})}{\sqrt{s}}, s, t)OutHeavisideTheta(2−t)πt\frac{\mathrm{HeavisideTheta}(2-t)}{\sqrt{π}\sqrt{t}}
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InInverseLaplaceTransform(EllipticK(a2s2)−π2,s,t)\mathrm{InverseLaplaceTransform}(\mathrm{EllipticK}(\frac{a^2}{s^2})-\frac{π}{2}, s, t)Out12(πaI⁡0(at2)I⁡1(at2))\frac{1}{2}(πa\operatorname{I}_{0}(\frac{at}{2})\operatorname{I}_{1}(\frac{at}{2}))
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InInverseLaplaceTransform(s×(π2−EllipticE(a2s2)),s,t)\mathrm{InverseLaplaceTransform}(s×(\frac{π}{2}-\mathrm{EllipticE}(\frac{a^2}{s^2})), s, t)OutπaI⁡0(at2)I⁡1(at2)2t\frac{πa\operatorname{I}_{0}(\frac{at}{2})\operatorname{I}_{1}(\frac{at}{2})}{2t}
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InInverseLaplaceTransform(1s+1,s,t)\mathrm{InverseLaplaceTransform}(\frac{1}{\sqrt{s+1}}, s, t)Outexp⁡(−t)πt\frac{\exp(-t)}{\sqrt{π}\sqrt{t}}
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InInverseLaplaceTransform(K⁡4(s)s2,s,t)\mathrm{InverseLaplaceTransform}(\frac{\operatorname{K}_{4}(\sqrt{s})}{s^2}, s, t)Out8t3exp⁡(−14t)8t^3\exp(-\frac{1}{4t})
About
Examples24
Checked againstWolfram Language 24 agree
CrosswalkWolfram Language

Implementation

primitive · kernela kernel — an algorithm over mutable state that would not be readable as a tree

nativeenginetypescriptpackages/symbols/analysis/analytic/src/transforms.ts

See also: LaplaceTransform, InverseFourierTransform