Initial value theorem

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Template:Short description 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)=∫0∞f(t)e−stdt

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

limt→0f(t)=lims→∞sF(s).

Proofs

Proof using dominated convergence theorem and assuming that function is bounded

Suppose first that f is bounded, i.e. limt→0+f(t)=α. A change of variable in the integral ∫0∞f(t)e−stdt shows that

sF(s)=∫0∞f(ts)e−tdt.

Since f is bounded, the Dominated Convergence Theorem implies that

lims→∞sF(s)=∫0∞αe−tdt=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 ∫A∞e−tdt<ϵ, and then note that lims→∞f(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)=e−ctf(t). Then g is bounded, so we've shown that g(0+)=lims→∞sG(s). But f(0+)=g(0+) and G(s)=F(s+c), so

lims→∞sF(s)=lims→∞(s−c)F(s)=lims→∞sF(s+c)=lims→∞sG(s),

since lims→∞F(s)=0.

See also

Notes

  1. ↑ Template:Cite book
  2. ↑ Robert H. Cannon, Dynamics of Physical Systems, Courier Dover Publications, 2003, page 567.


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