Laplace Transform of a periodic function

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The discussion focuses on deriving the Laplace transform of a periodic function f(t) with period T. The initial approach involves using the definition of the Laplace transform and recognizing the periodicity to express the integral as a sum over intervals. The goal is to manipulate this expression into a form resembling a geometric series, which is suggested as a potential solution pathway. A substitution is recommended to simplify the integral further, specifically using t = nT + u. The conversation emphasizes the importance of recognizing periodicity in transforming the function effectively.
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Homework Statement


Suppose f(t) is a periodic function with period T. Show that the Laplace transform of f is:

L(f) = \frac{1}{1-e^{-sT}}\int_0^T f(t)e^{-st} dt

The Attempt at a Solution


I started with the definition of a Laplace Transform for f:

L(f) = \int_0^\infty f(t)e^{-st}dt

Using the periodicity of the function this becomes:

\sum_{K=0}^\infty \int_{KT}^{(K+1)T} f(t)e^{-st}dt

At this point I have been trying to get this in the form of a geometric series, since the fraction in the final result leads me to look for a geometric series, but this has been without success. Any hints into the right direction to move from here on out would be appreciated. Thank you for any help you can offer.
 
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Try a substitution: t = nT+u with u as new variable.
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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