Visualizing the Laplace Transform (for beginners)












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I'm taking a differential equations course and have just been introduced to the concept of the Laplace Transform. I know its usefulness as a tool for solving IVPs, but I'm having trouble visualizing what the transform actually is. How would one explain the physical interpretation of the Laplace transform to a dummy? If possible, please refrain from using too much real/complex analysis (I only have experience in Linear Algebra, Multivariable Calculus, and Diff Eqs with some dabbling in function analysis).










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  • 3




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    I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
    $endgroup$
    – Kolja
    Jan 20 at 18:00










  • $begingroup$
    @Kolja Thank you so much! That video helped a ton with my understanding.
    $endgroup$
    – Hyperion
    Jan 21 at 16:34
















1












$begingroup$


I'm taking a differential equations course and have just been introduced to the concept of the Laplace Transform. I know its usefulness as a tool for solving IVPs, but I'm having trouble visualizing what the transform actually is. How would one explain the physical interpretation of the Laplace transform to a dummy? If possible, please refrain from using too much real/complex analysis (I only have experience in Linear Algebra, Multivariable Calculus, and Diff Eqs with some dabbling in function analysis).










share|cite|improve this question









$endgroup$








  • 3




    $begingroup$
    I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
    $endgroup$
    – Kolja
    Jan 20 at 18:00










  • $begingroup$
    @Kolja Thank you so much! That video helped a ton with my understanding.
    $endgroup$
    – Hyperion
    Jan 21 at 16:34














1












1








1





$begingroup$


I'm taking a differential equations course and have just been introduced to the concept of the Laplace Transform. I know its usefulness as a tool for solving IVPs, but I'm having trouble visualizing what the transform actually is. How would one explain the physical interpretation of the Laplace transform to a dummy? If possible, please refrain from using too much real/complex analysis (I only have experience in Linear Algebra, Multivariable Calculus, and Diff Eqs with some dabbling in function analysis).










share|cite|improve this question









$endgroup$




I'm taking a differential equations course and have just been introduced to the concept of the Laplace Transform. I know its usefulness as a tool for solving IVPs, but I'm having trouble visualizing what the transform actually is. How would one explain the physical interpretation of the Laplace transform to a dummy? If possible, please refrain from using too much real/complex analysis (I only have experience in Linear Algebra, Multivariable Calculus, and Diff Eqs with some dabbling in function analysis).







ordinary-differential-equations laplace-transform






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asked Jan 20 at 17:54









HyperionHyperion

636110




636110








  • 3




    $begingroup$
    I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
    $endgroup$
    – Kolja
    Jan 20 at 18:00










  • $begingroup$
    @Kolja Thank you so much! That video helped a ton with my understanding.
    $endgroup$
    – Hyperion
    Jan 21 at 16:34














  • 3




    $begingroup$
    I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
    $endgroup$
    – Kolja
    Jan 20 at 18:00










  • $begingroup$
    @Kolja Thank you so much! That video helped a ton with my understanding.
    $endgroup$
    – Hyperion
    Jan 21 at 16:34








3




3




$begingroup$
I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
$endgroup$
– Kolja
Jan 20 at 18:00




$begingroup$
I very highly recommend to watch this lecture given by Arthur Mattuck - youtube.com/watch?v=sZ2qulI6GEk. It explains the Laplace transform in a beautiful manner, and shows the intuition behind it.
$endgroup$
– Kolja
Jan 20 at 18:00












$begingroup$
@Kolja Thank you so much! That video helped a ton with my understanding.
$endgroup$
– Hyperion
Jan 21 at 16:34




$begingroup$
@Kolja Thank you so much! That video helped a ton with my understanding.
$endgroup$
– Hyperion
Jan 21 at 16:34










1 Answer
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The Laplace transform and the Fourier transform are closely related. One way to view them is to analyse what happens in convolution of a function with anexponential functions. Recall that convolution is defined as
$$ (f*g)(x) := int_{-infty}^infty f(t),g(x-t) dt. tag{1}$$
If we let $,g_s(x) := e^{s,x},,$ a nice test function, then
$$ (f*g_s)(x) = int_{-infty}^infty f(t),e^{s,(x-t)} dt =
e^{s, x}, (f*g_s)(0).tag{2}$$

Now notice that $,(f*g_s)(0),$ is just the bilateral Laplace transform of $,f(t).,$ A similar situation arises for the Fourier transform. One interpretation of this is that the linear transformation $, g to f*g,$ has exponential eigenvectors $,g_s,$ and the associated eigenvalue is the Laplace transform $,F(s) = (f*g_s)(0).$



As for visualization, you can consult the Wikipedia article on convolution for illustrative examples.






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    $begingroup$

    The Laplace transform and the Fourier transform are closely related. One way to view them is to analyse what happens in convolution of a function with anexponential functions. Recall that convolution is defined as
    $$ (f*g)(x) := int_{-infty}^infty f(t),g(x-t) dt. tag{1}$$
    If we let $,g_s(x) := e^{s,x},,$ a nice test function, then
    $$ (f*g_s)(x) = int_{-infty}^infty f(t),e^{s,(x-t)} dt =
    e^{s, x}, (f*g_s)(0).tag{2}$$

    Now notice that $,(f*g_s)(0),$ is just the bilateral Laplace transform of $,f(t).,$ A similar situation arises for the Fourier transform. One interpretation of this is that the linear transformation $, g to f*g,$ has exponential eigenvectors $,g_s,$ and the associated eigenvalue is the Laplace transform $,F(s) = (f*g_s)(0).$



    As for visualization, you can consult the Wikipedia article on convolution for illustrative examples.






    share|cite|improve this answer









    $endgroup$


















      0












      $begingroup$

      The Laplace transform and the Fourier transform are closely related. One way to view them is to analyse what happens in convolution of a function with anexponential functions. Recall that convolution is defined as
      $$ (f*g)(x) := int_{-infty}^infty f(t),g(x-t) dt. tag{1}$$
      If we let $,g_s(x) := e^{s,x},,$ a nice test function, then
      $$ (f*g_s)(x) = int_{-infty}^infty f(t),e^{s,(x-t)} dt =
      e^{s, x}, (f*g_s)(0).tag{2}$$

      Now notice that $,(f*g_s)(0),$ is just the bilateral Laplace transform of $,f(t).,$ A similar situation arises for the Fourier transform. One interpretation of this is that the linear transformation $, g to f*g,$ has exponential eigenvectors $,g_s,$ and the associated eigenvalue is the Laplace transform $,F(s) = (f*g_s)(0).$



      As for visualization, you can consult the Wikipedia article on convolution for illustrative examples.






      share|cite|improve this answer









      $endgroup$
















        0












        0








        0





        $begingroup$

        The Laplace transform and the Fourier transform are closely related. One way to view them is to analyse what happens in convolution of a function with anexponential functions. Recall that convolution is defined as
        $$ (f*g)(x) := int_{-infty}^infty f(t),g(x-t) dt. tag{1}$$
        If we let $,g_s(x) := e^{s,x},,$ a nice test function, then
        $$ (f*g_s)(x) = int_{-infty}^infty f(t),e^{s,(x-t)} dt =
        e^{s, x}, (f*g_s)(0).tag{2}$$

        Now notice that $,(f*g_s)(0),$ is just the bilateral Laplace transform of $,f(t).,$ A similar situation arises for the Fourier transform. One interpretation of this is that the linear transformation $, g to f*g,$ has exponential eigenvectors $,g_s,$ and the associated eigenvalue is the Laplace transform $,F(s) = (f*g_s)(0).$



        As for visualization, you can consult the Wikipedia article on convolution for illustrative examples.






        share|cite|improve this answer









        $endgroup$



        The Laplace transform and the Fourier transform are closely related. One way to view them is to analyse what happens in convolution of a function with anexponential functions. Recall that convolution is defined as
        $$ (f*g)(x) := int_{-infty}^infty f(t),g(x-t) dt. tag{1}$$
        If we let $,g_s(x) := e^{s,x},,$ a nice test function, then
        $$ (f*g_s)(x) = int_{-infty}^infty f(t),e^{s,(x-t)} dt =
        e^{s, x}, (f*g_s)(0).tag{2}$$

        Now notice that $,(f*g_s)(0),$ is just the bilateral Laplace transform of $,f(t).,$ A similar situation arises for the Fourier transform. One interpretation of this is that the linear transformation $, g to f*g,$ has exponential eigenvectors $,g_s,$ and the associated eigenvalue is the Laplace transform $,F(s) = (f*g_s)(0).$



        As for visualization, you can consult the Wikipedia article on convolution for illustrative examples.







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Jan 20 at 21:46









        SomosSomos

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