MHB What has been done here to simplify the integration

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The discussion revolves around the integration of the function $e^{-st}$, where the lecturer rewrote it as $\frac{d}{dt}e^{-st}$ and removed the $(-\frac{1}{s})$ factor. Participants clarify that this approach relates to the integration by parts method, which is a standard technique for such integrals. There is mention of a potential 'trick' to simplify the integration without using integration by parts, prompting a suggestion to inquire further with the lecturer. The key point is that the derivative of $e^{-st}$ is $-s e^{-st}$, allowing for the factor $-\frac{1}{s}$ to be factored out during integration. Overall, the conversation emphasizes understanding the integration process and the techniques involved.
nacho-man
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Please refer to the attached image.

My lecturer seems to have re-written $e^{-st}$ as $\frac{d}{dt}e^{-st}$ and taken out the $(-\frac{1}{s}$ which I do see is equivalent, but i am unsure how he goes from there onwards.

Although, e is the derivative of itself. how does he split the integral into two, despite there being a multiplication of the terms?
 

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nacho said:
Please refer to the attached image.

My lecturer seems to have re-written $e^{-st}$ as $\frac{d}{dt}e^{-st}$ and taken out the $(-\frac{1}{s}$ which I do see is equivalent, but i am unsure how he goes from there onwards.

Although, e is the derivative of itself. how does he split the integral into two, despite there being a multiplication of the terms?

Your lecturer has applied the 'integration by parts' rule...

Kind regards

$\chi$ $\sigma$
 
hah. thanks..
that was mildly embarrassing.

i didn't closely to see if he had done so. when he was talking in the lecture he mentioned that there was a 'trick' way to integrate this w/o integrating by parts or something along those lines.
 
nacho said:
hah. thanks..
that was mildly embarrassing.

i didn't closely to see if he had done so. when he was talking in the lecture he mentioned that there was a 'trick' way to integrate this w/o integrating by parts or something along those lines.

I would ask him again what it was he said. By-parts is certainly the standard way to integrate this, and it's not all that difficult, once you know how. I suppose you could set up tabular integration, but that's just a unified way of keeping track of by-parts. It wouldn't be worth it for only one application of by-parts.
 
The first step depends upon the fact that \frac{d(e^{-st})}{dt}= -s e^{-st} so that, dividing both sides by -s, e^{-st}= -\frac{1}{s}\frac{d(e^{-st})}{dt}.

Of course, since "s" is independent of the integration variable, t, we can take -\frac{1}{s} out of the integral.
 
There are probably loads of proofs of this online, but I do not want to cheat. Here is my attempt: Convexity says that $$f(\lambda a + (1-\lambda)b) \leq \lambda f(a) + (1-\lambda) f(b)$$ $$f(b + \lambda(a-b)) \leq f(b) + \lambda (f(a) - f(b))$$ We know from the intermediate value theorem that there exists a ##c \in (b,a)## such that $$\frac{f(a) - f(b)}{a-b} = f'(c).$$ Hence $$f(b + \lambda(a-b)) \leq f(b) + \lambda (a - b) f'(c))$$ $$\frac{f(b + \lambda(a-b)) - f(b)}{\lambda(a-b)}...

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