Function modulation and dilatation in a Laplace transform












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My question is about something incomplete in my lesson. I learnt about the modulation and the dilatation of a function in the Laplace transform but what if I have both in the same time?



For the modulation, I have the following relation:



$$
mathcal{L}[e^{-gamma t} f(t)] = mathcal{L}[f](z + gamma)
$$



For the dilatation, I have the following relation:



$$
mathcal{L}[f(lambda t)] = frac{1}{lambda} mathcal{L}[f](frac{z}{lambda})
$$



What if I have the following Laplace transform : $mathcal{L}[e^{gamma t} f(frac{t}{lambda})]$



Is the answer $lambda mathcal{L}[f](lambda z - gamma)$ or $lambda mathcal{L}[f](lambda(z - gamma))$?










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    0












    $begingroup$


    My question is about something incomplete in my lesson. I learnt about the modulation and the dilatation of a function in the Laplace transform but what if I have both in the same time?



    For the modulation, I have the following relation:



    $$
    mathcal{L}[e^{-gamma t} f(t)] = mathcal{L}[f](z + gamma)
    $$



    For the dilatation, I have the following relation:



    $$
    mathcal{L}[f(lambda t)] = frac{1}{lambda} mathcal{L}[f](frac{z}{lambda})
    $$



    What if I have the following Laplace transform : $mathcal{L}[e^{gamma t} f(frac{t}{lambda})]$



    Is the answer $lambda mathcal{L}[f](lambda z - gamma)$ or $lambda mathcal{L}[f](lambda(z - gamma))$?










    share|cite|improve this question









    $endgroup$















      0












      0








      0





      $begingroup$


      My question is about something incomplete in my lesson. I learnt about the modulation and the dilatation of a function in the Laplace transform but what if I have both in the same time?



      For the modulation, I have the following relation:



      $$
      mathcal{L}[e^{-gamma t} f(t)] = mathcal{L}[f](z + gamma)
      $$



      For the dilatation, I have the following relation:



      $$
      mathcal{L}[f(lambda t)] = frac{1}{lambda} mathcal{L}[f](frac{z}{lambda})
      $$



      What if I have the following Laplace transform : $mathcal{L}[e^{gamma t} f(frac{t}{lambda})]$



      Is the answer $lambda mathcal{L}[f](lambda z - gamma)$ or $lambda mathcal{L}[f](lambda(z - gamma))$?










      share|cite|improve this question









      $endgroup$




      My question is about something incomplete in my lesson. I learnt about the modulation and the dilatation of a function in the Laplace transform but what if I have both in the same time?



      For the modulation, I have the following relation:



      $$
      mathcal{L}[e^{-gamma t} f(t)] = mathcal{L}[f](z + gamma)
      $$



      For the dilatation, I have the following relation:



      $$
      mathcal{L}[f(lambda t)] = frac{1}{lambda} mathcal{L}[f](frac{z}{lambda})
      $$



      What if I have the following Laplace transform : $mathcal{L}[e^{gamma t} f(frac{t}{lambda})]$



      Is the answer $lambda mathcal{L}[f](lambda z - gamma)$ or $lambda mathcal{L}[f](lambda(z - gamma))$?







      laplace-transform






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      asked Dec 11 '18 at 12:53









      WizixWizix

      1032




      1032






















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          Define modulation and dilation operators: $M_{gamma}f(t) = e^{-gamma t} f(t)$ and $D_{lambda}f(t) = f(lambda t)$. Then $t mapsto e^{gamma t} f(t/lambda)$ can be expressed as either $M_{-gamma} (D_{1/lambda} f)$ (dilation then modulation) or $D_{1/lambda}(M_{-gamma lambda} f)$ (modulation then dilation). Using either form, we obtain the same result.
          $$mathcal L[M_{-gamma} (D_{1/lambda} f)](z) = mathcal L[D_{1/lambda} f](z gamma) = lambda mathcal L[f] (lambda(z - gamma))$$
          $$mathcal L[D_{1/lambda}(M_{-gamma lambda} f)](z) = lambda mathcal L[M_{-gamma lambda} f](lambda z) = lambda mathcal L[f] (lambda (z - gamma))$$






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            $begingroup$

            Define modulation and dilation operators: $M_{gamma}f(t) = e^{-gamma t} f(t)$ and $D_{lambda}f(t) = f(lambda t)$. Then $t mapsto e^{gamma t} f(t/lambda)$ can be expressed as either $M_{-gamma} (D_{1/lambda} f)$ (dilation then modulation) or $D_{1/lambda}(M_{-gamma lambda} f)$ (modulation then dilation). Using either form, we obtain the same result.
            $$mathcal L[M_{-gamma} (D_{1/lambda} f)](z) = mathcal L[D_{1/lambda} f](z gamma) = lambda mathcal L[f] (lambda(z - gamma))$$
            $$mathcal L[D_{1/lambda}(M_{-gamma lambda} f)](z) = lambda mathcal L[M_{-gamma lambda} f](lambda z) = lambda mathcal L[f] (lambda (z - gamma))$$






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              0












              $begingroup$

              Define modulation and dilation operators: $M_{gamma}f(t) = e^{-gamma t} f(t)$ and $D_{lambda}f(t) = f(lambda t)$. Then $t mapsto e^{gamma t} f(t/lambda)$ can be expressed as either $M_{-gamma} (D_{1/lambda} f)$ (dilation then modulation) or $D_{1/lambda}(M_{-gamma lambda} f)$ (modulation then dilation). Using either form, we obtain the same result.
              $$mathcal L[M_{-gamma} (D_{1/lambda} f)](z) = mathcal L[D_{1/lambda} f](z gamma) = lambda mathcal L[f] (lambda(z - gamma))$$
              $$mathcal L[D_{1/lambda}(M_{-gamma lambda} f)](z) = lambda mathcal L[M_{-gamma lambda} f](lambda z) = lambda mathcal L[f] (lambda (z - gamma))$$






              share|cite|improve this answer











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                0












                0








                0





                $begingroup$

                Define modulation and dilation operators: $M_{gamma}f(t) = e^{-gamma t} f(t)$ and $D_{lambda}f(t) = f(lambda t)$. Then $t mapsto e^{gamma t} f(t/lambda)$ can be expressed as either $M_{-gamma} (D_{1/lambda} f)$ (dilation then modulation) or $D_{1/lambda}(M_{-gamma lambda} f)$ (modulation then dilation). Using either form, we obtain the same result.
                $$mathcal L[M_{-gamma} (D_{1/lambda} f)](z) = mathcal L[D_{1/lambda} f](z gamma) = lambda mathcal L[f] (lambda(z - gamma))$$
                $$mathcal L[D_{1/lambda}(M_{-gamma lambda} f)](z) = lambda mathcal L[M_{-gamma lambda} f](lambda z) = lambda mathcal L[f] (lambda (z - gamma))$$






                share|cite|improve this answer











                $endgroup$



                Define modulation and dilation operators: $M_{gamma}f(t) = e^{-gamma t} f(t)$ and $D_{lambda}f(t) = f(lambda t)$. Then $t mapsto e^{gamma t} f(t/lambda)$ can be expressed as either $M_{-gamma} (D_{1/lambda} f)$ (dilation then modulation) or $D_{1/lambda}(M_{-gamma lambda} f)$ (modulation then dilation). Using either form, we obtain the same result.
                $$mathcal L[M_{-gamma} (D_{1/lambda} f)](z) = mathcal L[D_{1/lambda} f](z gamma) = lambda mathcal L[f] (lambda(z - gamma))$$
                $$mathcal L[D_{1/lambda}(M_{-gamma lambda} f)](z) = lambda mathcal L[M_{-gamma lambda} f](lambda z) = lambda mathcal L[f] (lambda (z - gamma))$$







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Dec 11 '18 at 14:08

























                answered Dec 11 '18 at 13:20









                Roberto RastapopoulosRoberto Rastapopoulos

                950425




                950425






























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