how to do derivative of transforms thingy? for example: show that \(\Large\mathcal L \lbrace t^{1/2} \rbrace = \frac{1}{2s} \left(\frac{\pi}{s}\right) ^{1/2}, \quad \quad s>0\)
for the record...i have no idea
Can you use Integration By Parts here: \[\large \mathsf{\int\limits\limits_{0}^{\infty} (t^\frac{1}{2}) \cdot (e^{-st})dt}\]
uhmm i have to use derivative of transforms instead of the usual..
By this we can find the derivative but I will give you directly how to derivative first time: \[\large \mathcal{L[f'(t)] = s \cdot L[f(t)] - }\textbf {f(0)}\]
??
Solve for RHS here..
i have no idea or background knowledge on derivative of transforms...
Find: \(\mathcal{L{f(t)}}\) first and then multiply it by s..
\[\large \mathcal{L(f(t)}) = \int\limits\limits _{0} ^{ \infty} (t^{\frac{1}{2}} \cdot e^{-st}) dt\]
\[\mathcal L\{f(t)\}=\int_0^∞f(t)e^{-st}\text dt\] \[\mathcal L\{t^{1/2}\}=\int_0^∞t^{1/2}e^{-st}\text dt\] \[=e^{-s}\int_0^∞t^{1/2}e^{t}\text dt\]\[=e^{-s}\Gamma \left( \frac{3}{2}\right)\]\[=e^{-s} \frac12\Gamma\left(\frac 12\right)\]\[=e^{-s}\frac {\sqrt{\pi}}{2}\] ive dones something wrong, but im sure this will help a bit
\[\large e^{-st} \ne e^{-s} \cdot e^{t}\]
..i still ahve no idea what you are saying o.O
i often try to do that even thought it is illegal
I mean how you separate \(e^{-st}\) from the integral ??
can someone tell me how to derive transforms first?
If it was: \[\large e^{-s +t} = e^{-s} \cdot e^{t}\] Then you can do this..
what should i have done after this \[\mathcal L\{t^{1/2}\}=\int_0^∞t^{1/2}e^{-st}\text dt\]\[\qquad\qquad=\]
We have to use here Integration By Parts..
maybe i should go and give you guys some space to discuss what you're discussing...
Can you check one thing @lgbasallote
i had no idea what any of you were saying...how can i check anything o.O
espansion? series? what??!
i dont know i havent studied laplace in a while, i dont think series expansion is a good idea, maybe completing the square ,
\[\large \int\limits\limits _{0} ^{\infty}(t^{\frac{-1}{2}} \cdot e^{-st}) dt = (\frac{\pi}{s})^{\frac{1}{2}}\] Here now @mukushla will help us..
what's going on here?? o.O
someone wanna tell me something =_=
you all have your own worlds -_-
@mukushla can you prove that I have written the integral above in my just last post..??
NOTE: im asking about derivative of transforms....
I am doing the same I guess..
i just need a demo on taking derivative of transform not some fancy tricks to display your awesomeness =_=
I am not awesome in laplace I was just helping you a bit in proving what you have written above..
yeah i know. i just love being sarcastic
i have no idea how to take the derivative of transform...i dont get what you linked me too..i hate links...
I also hate the links..
so how do you take derivativee of transforms?
i'll just try a simpler example...
well let \[F(s)=\int\limits_{0}^{\infty} f(t,s) dt\] then u can write \[\frac{dF}{ds}=\int\limits_{0}^{\infty} \frac{\partial f}{\partial s} dt\] if second integral is convergence...
ugh..not good with letters =_= i'll just ask a simpler question and maybe i can get a demo there
huh?? Out of my knowledge..
u just clarify us....derivative of transforms or transform of derivatives?
\[\mathcal L\{t^{1/2}\}=\int\limits\limits_0^∞ t^{1/2}e^{-st}\text dt \implies \left| - \frac{t^{\frac{1}{2}} \cdot e^{-st}}{s} \right|_0^{\infty} + \frac{1}{2s} \int\limits\limits _{0}^{\infty} t^{\frac{-1}{2}} \cdot e^{-st}dt\] .\[\large \implies 0 + \frac{1}{2s} \mathcal{L[t^{\frac{-1}{2}}]} \implies \frac{1}{2s} \frac{\Gamma (\frac{1}{2})}{s^{\frac{1}{2}}}\] \[\Gamma (\frac{1}{2}) = \sqrt{\pi}\] \[\large \mathcal{L[t^{\frac{1}{2}}]} = \frac{1}{2s} \sqrt{\frac{\pi}{s}}, \; \; s > 0\]
found the answer already...@sami-21 taught me gamma functions \m/
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