Show the equality of two expressions

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SUMMARY

The forum discussion focuses on demonstrating the equality of two mathematical expressions involving integrals and exponentials. The first expression, \sum_{k=0}^{N-1}e^{\gamma \tau k}\int_{0}^{\tau}F'(k\tau+s)ds, can be transformed into the second expression, \int_{0}^{t}e^{\gamma t'}F'(t')dt', by recognizing that the integral maintains the same statistical properties across intervals of length \tau. The discussion emphasizes the importance of substituting variables and moving the exponential into the integrand, particularly when considering the limit as N approaches infinity. The key equations referenced are t=N\tau and the statistical independence of the integrals.

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Homework Statement


Show that

\sum_{k=0}^{N-1}e^{\gamma \tau k}\int_{0}^{\tau}F'(k\tau+s)ds

can be written as

\int_{0}^{t}e^{\gamma t'}F'(t')dt'

Homework Equations



1. t=N\tau

2. \int_{0}^{\tau}F'(k\tau+s)ds has the same statistical properties for each interval of length \tau, and is statistically independent with respect to k.

The Attempt at a Solution


I barely know where to start. As a first step, I'm thinking that perhaps "same statistical properties" means that the integral is the same regardless of k, so that

\int_{0}^{\tau}F'(k\tau+s)ds=\int_{0}^{\tau}F'(s)ds,

i.e., k=0. Is this correct?
 
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Without the exponential, the first expression would just be a piecewise definition of the second integral, and a substitution would transform them into each other (can you see how? Hint: which argument values are used in F in the first, second, ... integral?). I guess you need the second relevant equation to get the same result including the exponential, but it could be still interesting to make that substitution.
 
mfb said:
Without the exponential, the first expression would just be a piecewise definition of the second integral, and a substitution would transform them into each other (can you see how? Hint: which argument values are used in F in the first, second, ... integral?). I guess you need the second relevant equation to get the same result including the exponential, but it could be still interesting to make that substitution.

Thanks. That gives me

\sum_{k=0}^{N-1}e^{\gamma \tau k}\int_{k\tau}^{(k+1)\tau}F'(t')dt'.

What's left now is to move the exponential into the integrand, but I'm not sure how that can be justified.
 
That I don't know. It does not work for general functions F', but it works if you take the limit N -> infinity (with finite t), and it might work for some special F' even with finite N.
 

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