Thursday, 27 February 2014

LAPLACE TRANSFORMATION

The Laplace transform of a function f(t), defined for all real numbers t ≥ 0, is the function F(s), defined by:



The parameter s is a complex number:
with real numbers σ and ω.
Other notations for the Laplace transform includeor alternativelyinstead of F.
The meaning of the integral depends on types of functions of interest. A necessary condition for existence of the integral is that f must be locally integrable on [0,∞). For locally integrable functions that decay at infinity or are of exponential type , the integral can be understood as a (proper) Lebesgue integral. However, for many applications it is necessary to regard it as a conditionally convergent improper integral at ∞. Still more generally, the integral can be understood in a weak sense, and this is dealt with below.
One can define the Laplace transform of a finite Borel measure μ by the Lebesgue integral.


An important special case is where μ is a probability measure or, even more specifically, the Dirac delta function. In operational calculus, the Laplace transform of a measure is often treated as though the measure came from a distribution function f. In that case, to avoid potential confusion, one often writes


where the lower limit of 0 is shorthand notation for


This limit emphasizes that any point mass located at 0 is entirely captured by the Laplace transform. Although with the Lebesgue integral, it is not necessary to take such a limit, it does appear more naturally in connection with the Laplace transform.
Probability theorem
the Laplace transform is defined as an expected value . If X is a random variable with probability density function f, then the Laplace transform of  f is given by the expectation


 this is referred to as the Laplace transform of the random variable X itself. Replacing s by −t gives the moment generating function of X. The Laplace transform has applications throughout probability theory, including first passage time of stochastic processes such As Markov chains , and renewal theory.
Of particular use is the ability to recover the cumulative distribution function of a random variable X by means of the Laplace transform as follow:


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