Finding the Laplace Transform of a Polynomial Function

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Homework Help Overview

The discussion revolves around finding the Laplace transform of the polynomial function \( t^2 - 2t \). Participants are exploring the correct approach to perform the transformation, particularly focusing on the integration process involved.

Discussion Character

  • Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply integration by parts to compute the Laplace transform but seems to confuse the variables of integration. Some participants question the correctness of integrating with respect to \( s \) instead of \( t \), suggesting a need to switch the differential.

Discussion Status

There is an ongoing exchange regarding the proper method for integrating the function. Some guidance has been offered about the variable of integration, indicating a potential direction for the original poster to reconsider their approach.

Contextual Notes

Participants are navigating the specifics of the integration process and the implications of variable choice in the context of Laplace transforms. There is an acknowledgment of confusion regarding the setup of the problem.

kidi3
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Homework Statement


Find the Laplace transform of the following function
t2 - 2t

The Attempt at a Solution


\[\begin{gathered}<br /> f\left( t \right) = {t^2} - 2t \hfill \\<br /> l\left( {f\left( t \right)} \right) = F\left( s \right) = \int_0^\infty {{e^{ - st}} \cdot \left( {{t^2} - 2t} \right)ds} \hfill \\<br /> \Leftrightarrow \hfill \\<br /> = \int_0^\infty {{e^{ - st}}{t^2} - 2t{e^{ - st}}ds} \hfill \\<br /> = \int_0^\infty {{e^{ - st}}{t^2}} ds - \int_0^\infty {2t{e^{ - st}}} ds \hfill \\<br /> = \int_0^\infty {{e^{ - st}}{t^2}} ds - \int_0^\infty {2t{e^{ - st}}} ds \hfill \\<br /> {\text{Integration by parts}} \hfill \\<br /> \int_0^\infty {{e^{ - st}}{t^2}} ds \hfill \\<br /> \int_{}^{} {uv&#039; = uv - \int_{}^{} {u&#039;v} } \hfill \\<br /> v&#039;\left( t \right) = {e^{ - st}} \Rightarrow v = \frac{{ - 1}}{s}{e^{ - st}} \hfill \\<br /> u\left( t \right) = {t^2} \Rightarrow u&#039;\left( t \right) = 2t \hfill \\<br /> \int_{}^{} {uv&#039; = uv - \int_{}^{} {u&#039;v} } \hfill \\<br /> \int_0^\infty {{e^{ - st}}{t^2}} ds = \frac{{ - 1}}{s}{e^{ - st}} \cdot {t^2} - \int_{}^{} {2t \cdot } \frac{{ - 1}}{s}{e^{ - st}}ds = \frac{{ - 1}}{s}{e^{ - st}} \cdot {t^2} - \frac{{ - 2}}{s}\int_{}^{} {t \cdot } {e^{ - st}}ds \hfill \\ <br /> \end{gathered} \]am i doing it correctly?
 
Last edited:
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You're supposed to integrate with respect to ##t##, not ##s##! Switch the ##ds## with ##dt## and start over.
 
Ahh.. It makes sense now.
 
Could you tell me what i am doing wrong with this one..

Think i got it..
 
Last edited:

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