Initial value theorem
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
- {\displaystyle F(s)=\int _{0}^{\infty }f(t)e^{-st},円dt}
be the (one-sided) Laplace transform of ƒ(t). If {\displaystyle f} is bounded on {\displaystyle (0,\infty )} (or if just {\displaystyle f(t)=O(e^{ct})}) and {\displaystyle \lim _{t\to 0^{+}}f(t)} exists then the initial value theorem says[2]
- {\displaystyle \lim _{t,円\to ,0円}f(t)=\lim _{s\to \infty }{sF(s)}.}
Proofs
[edit ]Proof using dominated convergence theorem and assuming that function is bounded
[edit ]Suppose first that {\displaystyle f} is bounded, i.e. {\displaystyle \lim _{t\to 0^{+}}f(t)=\alpha }. A change of variable in the integral {\displaystyle \int _{0}^{\infty }f(t)e^{-st},円dt} shows that
- {\displaystyle sF(s)=\int _{0}^{\infty }f\left({\frac {t}{s}}\right)e^{-t},円dt}.
Since {\displaystyle f} is bounded, the Dominated Convergence Theorem implies that
- {\displaystyle \lim _{s\to \infty }sF(s)=\int _{0}^{\infty }\alpha e^{-t},円dt=\alpha .}
Proof using elementary calculus and assuming that function is bounded
[edit ]Of course we don't really need DCT here, one can give a very simple proof using only elementary calculus:
Start by choosing {\displaystyle A} so that {\displaystyle \int _{A}^{\infty }e^{-t},円dt<\epsilon }, and then note that {\displaystyle \lim _{s\to \infty }f\left({\frac {t}{s}}\right)=\alpha } uniformly for {\displaystyle t\in (0,A]}.
Generalizing to non-bounded functions that have exponential order
[edit ]The theorem assuming just that {\displaystyle f(t)=O(e^{ct})} follows from the theorem for bounded {\displaystyle f}:
Define {\displaystyle g(t)=e^{-ct}f(t)}. Then {\displaystyle g} is bounded, so we've shown that {\displaystyle g(0^{+})=\lim _{s\to \infty }sG(s)}. But {\displaystyle f(0^{+})=g(0^{+})} and {\displaystyle G(s)=F(s+c)}, so
- {\displaystyle \lim _{s\to \infty }sF(s)=\lim _{s\to \infty }(s-c)F(s)=\lim _{s\to \infty }sF(s+c)=\lim _{s\to \infty }sG(s),}
since {\displaystyle \lim _{s\to \infty }F(s)=0}.
See also
[edit ]Notes
[edit ]- ^ Fourier and Laplace transforms. R. J. Beerends. Cambridge: Cambridge University Press. 2003. ISBN 978-0-511-67510-2. OCLC 593333940.
{{cite book}}
: CS1 maint: others (link) - ^ Robert H. Cannon, Dynamics of Physical Systems, Courier Dover Publications, 2003, page 567.
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