Solve a wave equation using D'Alembert solution.











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Solve the PDE:



$begin{equation}
frac{partial^2u}{partial t^2} - frac{partial ^2 u}{partial x^2}=0, qquad 0<x<L,quad t>0 \
u(x,0)=f(x) qquad frac{partial u}{partial t }(x,0)=g(x)
end{equation}$



Find $u(x,t)$ for the values $f(x)=sin x$, $quad g(x)=0$ when $u(0,t)= 0$ and $frac{partial u}{partial x}(pi /2,t)=0$



My attempt



We know the PDE is only a wave equation, then applying D'Alembert formula we have:



$u(x,t)=frac{1}{2}[f(x-ct)+f(x+ct)]+frac{1}{2c}int^{x+ct}_{x-ct}g(s)ds. tag 1$



As $g(x)=$0 then $(1)$ is:



$u(x,t)=frac{1}{2}[f(x-t)+f(x+t)] tag 1$



Note we have a Neumman condition the we need make even periodic extension



Then
begin{equation}
f(x) = left{
begin{array}{ll}
sin(x) & mathrm{if } 0<x<frac{pi}{2} \
-sin(x) & mathrm{if } -frac{pi}{2}<x<0 \
end{array}
right.
end{equation}



such that $f(x pm pi/2)=f(x)$



This implies:



$
begin{equation}
f(x-t) = left{
begin{array}{ll}
sin(x-t) & mathrm{if } 0<x<frac{pi}{2} \
-sin(x-t) & mathrm{if } -frac{pi}{2}<x<0 \
end{array}
right.
end{equation}
$



and



$
begin{equation}
f(x+t) = left{
begin{array}{ll}
sin(x+t) & mathrm{if } 0<x<frac{pi}{2} \
-sin(x+t) & mathrm{if } -frac{pi}{2}<x<0 \
end{array}
right.
end{equation}
$



Is correct this?










share|cite|improve this question


























    up vote
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    down vote

    favorite
    2












    Solve the PDE:



    $begin{equation}
    frac{partial^2u}{partial t^2} - frac{partial ^2 u}{partial x^2}=0, qquad 0<x<L,quad t>0 \
    u(x,0)=f(x) qquad frac{partial u}{partial t }(x,0)=g(x)
    end{equation}$



    Find $u(x,t)$ for the values $f(x)=sin x$, $quad g(x)=0$ when $u(0,t)= 0$ and $frac{partial u}{partial x}(pi /2,t)=0$



    My attempt



    We know the PDE is only a wave equation, then applying D'Alembert formula we have:



    $u(x,t)=frac{1}{2}[f(x-ct)+f(x+ct)]+frac{1}{2c}int^{x+ct}_{x-ct}g(s)ds. tag 1$



    As $g(x)=$0 then $(1)$ is:



    $u(x,t)=frac{1}{2}[f(x-t)+f(x+t)] tag 1$



    Note we have a Neumman condition the we need make even periodic extension



    Then
    begin{equation}
    f(x) = left{
    begin{array}{ll}
    sin(x) & mathrm{if } 0<x<frac{pi}{2} \
    -sin(x) & mathrm{if } -frac{pi}{2}<x<0 \
    end{array}
    right.
    end{equation}



    such that $f(x pm pi/2)=f(x)$



    This implies:



    $
    begin{equation}
    f(x-t) = left{
    begin{array}{ll}
    sin(x-t) & mathrm{if } 0<x<frac{pi}{2} \
    -sin(x-t) & mathrm{if } -frac{pi}{2}<x<0 \
    end{array}
    right.
    end{equation}
    $



    and



    $
    begin{equation}
    f(x+t) = left{
    begin{array}{ll}
    sin(x+t) & mathrm{if } 0<x<frac{pi}{2} \
    -sin(x+t) & mathrm{if } -frac{pi}{2}<x<0 \
    end{array}
    right.
    end{equation}
    $



    Is correct this?










    share|cite|improve this question
























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      up vote
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      down vote

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      Solve the PDE:



      $begin{equation}
      frac{partial^2u}{partial t^2} - frac{partial ^2 u}{partial x^2}=0, qquad 0<x<L,quad t>0 \
      u(x,0)=f(x) qquad frac{partial u}{partial t }(x,0)=g(x)
      end{equation}$



      Find $u(x,t)$ for the values $f(x)=sin x$, $quad g(x)=0$ when $u(0,t)= 0$ and $frac{partial u}{partial x}(pi /2,t)=0$



      My attempt



      We know the PDE is only a wave equation, then applying D'Alembert formula we have:



      $u(x,t)=frac{1}{2}[f(x-ct)+f(x+ct)]+frac{1}{2c}int^{x+ct}_{x-ct}g(s)ds. tag 1$



      As $g(x)=$0 then $(1)$ is:



      $u(x,t)=frac{1}{2}[f(x-t)+f(x+t)] tag 1$



      Note we have a Neumman condition the we need make even periodic extension



      Then
      begin{equation}
      f(x) = left{
      begin{array}{ll}
      sin(x) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}



      such that $f(x pm pi/2)=f(x)$



      This implies:



      $
      begin{equation}
      f(x-t) = left{
      begin{array}{ll}
      sin(x-t) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x-t) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}
      $



      and



      $
      begin{equation}
      f(x+t) = left{
      begin{array}{ll}
      sin(x+t) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x+t) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}
      $



      Is correct this?










      share|cite|improve this question













      Solve the PDE:



      $begin{equation}
      frac{partial^2u}{partial t^2} - frac{partial ^2 u}{partial x^2}=0, qquad 0<x<L,quad t>0 \
      u(x,0)=f(x) qquad frac{partial u}{partial t }(x,0)=g(x)
      end{equation}$



      Find $u(x,t)$ for the values $f(x)=sin x$, $quad g(x)=0$ when $u(0,t)= 0$ and $frac{partial u}{partial x}(pi /2,t)=0$



      My attempt



      We know the PDE is only a wave equation, then applying D'Alembert formula we have:



      $u(x,t)=frac{1}{2}[f(x-ct)+f(x+ct)]+frac{1}{2c}int^{x+ct}_{x-ct}g(s)ds. tag 1$



      As $g(x)=$0 then $(1)$ is:



      $u(x,t)=frac{1}{2}[f(x-t)+f(x+t)] tag 1$



      Note we have a Neumman condition the we need make even periodic extension



      Then
      begin{equation}
      f(x) = left{
      begin{array}{ll}
      sin(x) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}



      such that $f(x pm pi/2)=f(x)$



      This implies:



      $
      begin{equation}
      f(x-t) = left{
      begin{array}{ll}
      sin(x-t) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x-t) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}
      $



      and



      $
      begin{equation}
      f(x+t) = left{
      begin{array}{ll}
      sin(x+t) & mathrm{if } 0<x<frac{pi}{2} \
      -sin(x+t) & mathrm{if } -frac{pi}{2}<x<0 \
      end{array}
      right.
      end{equation}
      $



      Is correct this?







      pde






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      asked Nov 12 at 16:28









      Bvss12

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