Initial value theorem

From HandWiki

In mathematical analysis, the initial value theorem is a theorem used to relate frequency domain expressions to the time domain behavior as time approaches zero.[1] Let

F(s)=0f(t)estdt

be the (one-sided) Laplace transform of ƒ(t). If f is bounded on (0,) (or if just f(t)=O(ect)) and limt0+f(t) exists then the initial value theorem says[2]

limt0f(t)=limssF(s).

Proofs

Proof using dominated convergence theorem and assuming that function is bounded

Suppose first that f is bounded, i.e. limt0+f(t)=α. A change of variable in the integral 0f(t)estdt shows that

sF(s)=0f(ts)etdt.

Since f is bounded, the Dominated Convergence Theorem implies that

limssF(s)=0αetdt=α.

Proof using elementary calculus and assuming that function is bounded

Of course we don't really need DCT here, one can give a very simple proof using only elementary calculus:

Start by choosing A so that Aetdt<ϵ, and then note that limsf(ts)=α uniformly for t(0,A].

Generalizing to non-bounded functions that have exponential order

The theorem assuming just that f(t)=O(ect) follows from the theorem for bounded f:

Define g(t)=ectf(t). Then g is bounded, so we've shown that g(0+)=limssG(s). But f(0+)=g(0+) and G(s)=F(s+c), so

limssF(s)=lims(sc)F(s)=limssF(s+c)=limssG(s),

since limsF(s)=0.

See also

Notes

  1. Fourier and Laplace transforms. R. J. Beerends. Cambridge: Cambridge University Press. 2003. ISBN 978-0-511-67510-2. OCLC 593333940. https://www.worldcat.org/oclc/593333940. 
  2. Robert H. Cannon, Dynamics of Physical Systems, Courier Dover Publications, 2003, page 567.