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Calculus

Laplace Transform

A table of common Laplace transforms with the Gamma function and notes on hyperbolic trigonometric forms.

The Laplace transform maps a time-domain function f(t) to a complex-frequency-domain function F(s) by an exponential-weighted integral, converting differential equations into algebraic ones. It turns differentiation into multiplication by s (with initial-value terms), so linear ODEs with constant coefficients become rational equations in s. The solution is recovered by inverse-transforming back to the t domain via the table or partial fractions. The transform is linear. Entries 24-26 give the scaling and shifting rules: frequency-shift by an exponential factor in t, time-shift by multiplication by e-cs in s. The table pairs each f(t) with its F(s). Reading right-to-left gives the inverse transform.

f(t)time domainF(s)frequency domainℒℒ⁻¹
The Laplace transform maps a time-domain function to a frequency-domain function.
#f(t)=L−1{F(s)}f\left(t\right)=L^{-1}\left\{F\left(s\right)\right\}F(s)=L{f(t)}F\left(s\right)=L\left\{f\left(t\right)\right\}
111s\frac{1}{s}
2eate^{at}1s−a\frac{1}{s-a}
3tn    (n=1,2,3...)t^{n}\text{ }\text{ }\text{ }\text{ }\left(n=1,2,3...\right)n!s(n+1)\frac{n!}{s^{\left(n+1\right)}}
4tp(p>−1)t^{p}\left(p>-1\right)⌜(p+1)s(p+1)\frac{\ulcorner\left(p+1\right)}{s^{\left(p+1\right)}}
5t\sqrt{t}π2 s32\frac{\sqrt{\pi}}{2\text{ }s^{\frac{3}{2}}}
6tn−12   (n=1,2,3...)t^{\frac{n-1}{2}}\text{ }\text{ }\text{ }\left(n=1,2,3...\right)1×3×5...(2n−1)π2nsn+12\frac{1\times3\times5...\left(2n-1\right)\sqrt{\pi}}{2^{n}s^{\frac{n+1}{2}}}
7sin⁡(at)\sin\left(at\right)as2+a2\frac{a}{s^{2}+a^{2}}
8cos⁡(at)\cos\left(at\right)ss2+a2\frac{s}{s^{2}+a^{2}}
9t sin⁡(at)t\text{ }\sin\left(at\right)2as(s2+a2)2\frac{2as}{\left(s^{2}+a^{2}\right)^{2}}
10t cos⁡(at)t\text{ }\cos\left(at\right)s2−a2(s2+a2)2\frac{s^{2}-a^{2}}{\left(s^{2}+a^{2}\right)^{2}}
11sin⁡(at)−at cos⁡(at)\sin\left(at\right)-at\text{ }\cos\left(at\right)2a3(s2+a2)2\frac{2a^{3}}{\left(s^{2}+a^{2}\right)^{2}}
12sin⁡(at)+at cos⁡(at)\sin\left(at\right)+at\text{ }\cos\left(at\right)2as2(s2+a2)2\frac{2as^{2}}{\left(s^{2}+a^{2}\right)^{2}}
13cos⁡(at)−at sin(at)\cos\left(at\right)-at\text{ }sin\left(at\right)s(s2−a2)(s2+a2)2\frac{s\left(s^{2}-a^{2}\right)}{\left(s^{2}+a^{2}\right)^{2}}
14cos⁡(at)+at sin(at)\cos\left(at\right)+at\text{ }sin\left(at\right)s(s2+3a2)(s2+a2)2\frac{s\left(s^{2}+3a^{2}\right)}{\left(s^{2}+a^{2}\right)^{2}}
15sin⁡(at+b)\sin\left(at+b\right)s sin⁡(b)+a cos⁡(b)s2+a2\frac{s\text{ }\sin\left(b\right)+a\text{ }\cos\left(b\right)}{s^{2}+a^{2}}
16cos⁡(at+b)\cos\left(at+b\right)s cos⁡(b)−a sin⁡(b)s2+a2\frac{s\text{ }\cos\left(b\right)-a\text{ }\sin\left(b\right)}{s^{2}+a^{2}}
17sinh⁡(at)\sinh\left(at\right)as2−a2\frac{a}{s^{2}-a^{2}}
18cosh⁡(at)\cosh\left(at\right)ss2−a2\frac{s}{s^{2}-a^{2}}
19eatsin⁡(bt)e^{at}\sin\left(bt\right)b(s−a)2+b\frac{b}{\left(s-a\right)^{2}+b}
20eatcos⁡(bt)e^{at}\cos\left(bt\right)s−a(s−a)2+b\frac{s-a}{\left(s-a\right)^{2}+b}
21eatsinh⁡(bt)e^{at}\sinh\left(bt\right)b(s−a)2−b\frac{b}{\left(s-a\right)^{2}-b}
22eatcosh⁡(bt)e^{at}\cosh\left(bt\right)s−a(s−a)2−b\frac{s-a}{\left(s-a\right)^{2}-b}
23tneat    (n=1,2,3...)t^{n}e^{at}\text{ }\text{ }\text{ }\text{ }\left(n=1,2,3...\right)n!(s−a)(n+1)\frac{n!}{\left(s-a\right)^{\left(n+1\right)}}
24f(ct)f\left(ct\right)(1c)F(sc)\left(\frac{1}{c}\right)F\left(\frac{s}{c}\right)
25uc(t)=u(t−c)u_{c}\left(t\right)=u\left(t-c\right)e−css\frac{e^{-cs}}{s}
26℘(t−c)\wp\left(t-c\right)e−cse^{-cs}

Notes:

  1. The list is not inclusive and only contauin some of the most commonly used Laplace transforms and Formulase.

  2. deffinition of hyperbolic functions

The hyperbolic functions in entries 17-22:

 cosh⁡(t)=et+e−t2 , \text{ }\cosh\left(t\right)=\frac{e^{t}+e^{-t}}{2}\text{ }\text{, }
 sinh⁡(t)=et+e−t2 \text{ }\sinh\left(t\right)=\frac{e^{t}+e^{-t}}{2}\text{ }
  1. Be coreful while using “normal” trigonometric function vs hyperbolic trigonometric function. The only difference in the formaulas is “+a2” forthe “normal” trigonometric functions becomes “+a2” for the hyperbolic trigonometric functions.

  2. Formula #4 uses Gamma Function which is defined as

The Gamma function extends the factorial to non-integer arguments:

 ⌜(t)=∫O∞e−txt−1dx \text{ }\ulcorner\left(t\right)=\int_{O}^{\infty} e^{-t}x^{t-1}dx\text{ }

if n is a positive intrger then,

At positive integers it reduces to the factorial:

 ⌜(n+1)=n! \text{ }\ulcorner\left(n+1\right)=n!\text{ }

The Gamma function extends the normal factorial. Two quick facts.

Recurrence relation:

⌜(p+1)=p⌜(p)p(p+1)(p+1)...(p+n−1)=⌜(p+2)⌜(p)\ulcorner\left(p+1\right)=p\ulcorner\left(p\right)p\left(p+1\right)\left(p+1\right)...\left(p+n-1\right)=\frac{\ulcorner\left(p+2\right)}{\ulcorner\left(p\right)}

Half-integer value:

⌜(12)=π\ulcorner\left(\frac{1}{2}\right)=\sqrt{\pi}