Laplace transform of periodic functions


Let f⁢(t) be periodic with the positive period (http://planetmath.org/PeriodicFunctions) p.  Denote by H⁢(t) the Heaviside step function.  If now

g⁢(t):=f⁢(t)⁢H⁢(t)-f⁢(t-p)⁢H⁢(t-p),

then it follows

g⁢(t)={f⁢(t) for⁢  0<t<p,0   otherwise. (1)

By the parent entry (http://planetmath.org/DelayTheorem), the Laplace transformMathworldPlanetmath of g is

G⁢(s)=F⁢(s)-e-p⁢s⁢F⁢(s),

whence

F⁢(s)=G⁢(s)1-e-p⁢s=11-e-p⁢s⁢∫0∞e-s⁢t⁢g⁢(t)⁢𝑑t=11-e-p⁢s⁢∫0pe-s⁢t⁢f⁢(t)⁢𝑑t.

Thus we have the rule

ℒ⁢{f⁢(t)}=11-e-p⁢s⁢∫0pe-s⁢t⁢f⁢(t)⁢𝑑t  (period ⁢p). (2)

On the contrary, if f⁢(t) is antiperiodic with positive antiperiod p, then the function

g⁢(t):=f⁢(t)⁢H⁢(t)+f⁢(t-p)⁢H⁢(t-p)

also has the property (1).  Analogically with the preceding procedure, one may derive the rule

ℒ⁢{f⁢(t)}=11+e-p⁢s⁢∫0pe-s⁢t⁢f⁢(t)⁢𝑑t  (antiperiod ⁢p). (3)
Title Laplace transform of periodic functions
Canonical name LaplaceTransformOfPeriodicFunctions
Date of creation 2013-03-22 18:58:24
Last modified on 2013-03-22 18:58:24
Owner pahio (2872)
Last modified by pahio (2872)
Numerical id 5
Author pahio (2872)
Entry type Derivation
Classification msc 44A10
Related topic RectificationOfAntiperiodicFunction
Related topic TableOfLaplaceTransforms