Proof of the convolution theorem for laplace transform

Click For Summary
The discussion revolves around the proof of the convolution theorem for the Laplace transform, specifically questioning the change of variables in the proof. The user understands the overall concept of deriving the convolution of two Laplace transforms but is confused about why the variables for f(t) and g(t) are altered to f(a) and g(b) in the proof. The mathematical representation involves double integrals and a change of variables that leads to the conclusion that the Laplace transform of the convolution equals the product of the individual transforms. There is also a query about whether the limits of integration should be from 0 to t instead of 0 to infinity. The conversation highlights the intricacies of applying the convolution theorem in Laplace transforms.
O.J.
Messages
198
Reaction score
0
My textbook provides a proof but there's one thing about the proof i do not understand

it starts assuming L{f(t)} = the laplace integral with the f(t) changed to f(a)

same goes with L{g(t)} as it changes it to g(b)

i understand the big picture>>starting from a product of 2 L transforms and working ur way back to an expression in terms of the two functions transformed, but how can u change the variable for f and g when we started off stating f of T and g of T.?
 
Physics news on Phys.org
Am I not presenting my questions clearly?
 
Let

F(s)=\mathcal{L}\{f(t)\}=\int_0^{+\infty}e^{-s\,t}\,d\,t\,f(t) \quad \text{and} \quad <br /> G(s)=\mathcal{L}\{g(t)\}=\int_0^{+\infty}e^{-s\,t}\,g(t)\,d\,t

be the two Laplace transormations and let's denote

(f\star g)(t)=\int_0^{+\infty}f(\tau)\,g(t-\tau)\,d\,\tau

the convolution of f,\,g.

Thus the Laplace transform for the convolution would be

\mathcal{L}\{(f\star g)(t)\}=\int_0^{+\infty}e^{-s\,t}\left( \int_0^{+\infty}f(\tau)\,g(t-\tau)\,d\,\tau \right)\,d\,t =\int_0^{+\infty}\int_0^{+\infty}e^{-s\,t}f(\tau)\,g(t-\tau)\,d\,\tau \,d\,t \quad (1)

The above double integral is to be evaluated in the domain \mathcal{D}=\{(t,\tau): t \in (0,+\infty),\tau \in (0,+\infty)\}.

Performing the change of variables
(t,\tau)\rightarrow (u,v): t=u+v, \, \tau=v with u \in (0,+\infty),v \in (0,+\infty) we have d\,\tau\,d\,t=d\,u\,d\,v since the Jacobian equals to 1. Thus (1) becomes

\mathcal{L}\{(f\star g)(t)\}=\int_0^{+\infty}\int_0^{+\infty}e^{-s\,(u+v)}f(u)\,g(v)\,d\,u\,d\,v= \int_0^{+\infty}e^{-s\,u}f(u)\,d\,u \cdot \int_0^{+\infty}e^{-s\,v}\,g(v)\,d\,v

yielding to

\mathcal{L}\{(f\star g)(t)\}=\mathcal{L}\{f(t)\} \cdot \mathcal{L}\{g(t)\}

Nothing but double integrals! :smile:
 
  • Like
Likes davidbenari
Isn't the laplace convolution between 0 and t rather than 0 and infinity?
 

Similar threads

  • · Replies 17 ·
Replies
17
Views
3K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 7 ·
Replies
7
Views
6K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
7K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K