Solve Laplace Transform: t{e^{ - t}}u(t - 1)

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SUMMARY

The Laplace transform of the function t{e^{ - t}}u(t - 1) can be computed using established theorems rather than direct integration. The relevant theorems include the properties that relate the Laplace transform of a product of functions and the shifting theorem for unit step functions. Specifically, the transform can be derived as L(te^{-t}u(t-1)) = -\frac{d}{ds}\left(\frac{e^{-(s+1)}}{s+1}\right), resulting in the expression \frac{e^{-s+1}(s+1)+e^{-s+1}}{(s+1)^2}. This method simplifies the calculation and avoids complex integration techniques.

PREREQUISITES
  • Understanding of Laplace transforms and their properties
  • Familiarity with the unit step function u(t)
  • Knowledge of differentiation with respect to the Laplace variable s
  • Basic integration techniques, particularly integration by parts
NEXT STEPS
  • Study the properties of Laplace transforms, particularly the shifting theorem
  • Learn about the differentiation property of Laplace transforms
  • Explore examples of Laplace transforms involving the unit step function
  • Practice solving Laplace transforms using integration by parts and compare results
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Students studying differential equations, engineers working with control systems, and mathematicians interested in transform techniques will benefit from this discussion.

p75213
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Homework Statement


Is there an easier way of solving this rather than doing the integral?
Find the laplace transform of:

[tex]t{e^{ - t}}u(t - 1)[/tex]



Homework Equations





The Attempt at a Solution


[tex]\int_1^\infty {t{e^{ - t}}} {e^{ - st}}dt = \int_1^\infty {t{e^{ - t(1 + s)}}} dt = \frac{{{e^{ - (s + 1)}}}}{{{{(1 + s)}^2}}} + \frac{{{e^{ - (s + 1)}}}}{{1 + s}}[/tex]
 
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p75213 said:

Homework Statement


Is there an easier way of solving this rather than doing the integral?
Find the laplace transform of:

[tex]t{e^{ - t}}u(t - 1)[/tex]


The Attempt at a Solution


[tex]\int_1^\infty {t{e^{ - t}}} {e^{ - st}}dt = \int_1^\infty {t{e^{ - t(1 + s)}}} dt = \frac{{{e^{ - (s + 1)}}}}{{{{(1 + s)}^2}}} + \frac{{{e^{ - (s + 1)}}}}{{1 + s}}[/tex]
]

That integral isn't that tough, but if you prefer, you can use some of the theorems. For example, you have, if ##\mathcal L(f(t)) = F(s)## then ##\mathcal L(tf(t))=-F'(s)##. Also, ##\mathcal L(e^{at}f(t) = F(s-a)## and ##\mathcal L(u(t-1))=\frac{e^{-s}}{s}##.

So starting with ##\mathcal L(u(t-1))=\frac{e^{-s}}{s}= F(s)##, then ##\mathcal Le^{-t}u(t-1)=F(s+1) =\frac{e^{-(s+1)}}{s+1}## and $$L(te^{-t}u(t-1)) = -\frac d {ds}\left(\frac{e^{-(s+1)}}{s+1}\right)=\frac{e^{-s+1}(s+1)+e^{-s+1}}{(s+1)^2}$$which is the same answer.
 
True - it isn't that tough. But I am not so keen on integration by parts if I can avoid it.
Thanks for the reply.
 

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