Method of characteristics for system of linear transport equations












0












$begingroup$


If I have a system of pde
$$begin{cases}
u_t+v_x=0\
v_t+u_x=0\
u(x,0)=u_0(x), v(x,0)=v_0(x)end{cases}$$

how to extend the idea of method of characteristics to this situation? How do I parametrize the initial data and write the explicit solution to the problem for all $x$ and $t$ in terms of the functions $u_0$ and $v_0$?










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  • 1




    $begingroup$
    A great solution to method of characteristics for a system of PDEs is given here.
    $endgroup$
    – Mattos
    Nov 15 '18 at 3:47
















0












$begingroup$


If I have a system of pde
$$begin{cases}
u_t+v_x=0\
v_t+u_x=0\
u(x,0)=u_0(x), v(x,0)=v_0(x)end{cases}$$

how to extend the idea of method of characteristics to this situation? How do I parametrize the initial data and write the explicit solution to the problem for all $x$ and $t$ in terms of the functions $u_0$ and $v_0$?










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    A great solution to method of characteristics for a system of PDEs is given here.
    $endgroup$
    – Mattos
    Nov 15 '18 at 3:47














0












0








0


1



$begingroup$


If I have a system of pde
$$begin{cases}
u_t+v_x=0\
v_t+u_x=0\
u(x,0)=u_0(x), v(x,0)=v_0(x)end{cases}$$

how to extend the idea of method of characteristics to this situation? How do I parametrize the initial data and write the explicit solution to the problem for all $x$ and $t$ in terms of the functions $u_0$ and $v_0$?










share|cite|improve this question











$endgroup$




If I have a system of pde
$$begin{cases}
u_t+v_x=0\
v_t+u_x=0\
u(x,0)=u_0(x), v(x,0)=v_0(x)end{cases}$$

how to extend the idea of method of characteristics to this situation? How do I parametrize the initial data and write the explicit solution to the problem for all $x$ and $t$ in terms of the functions $u_0$ and $v_0$?







pde systems-of-equations hyperbolic-equations linear-pde






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share|cite|improve this question













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edited Dec 9 '18 at 12:56









Harry49

6,43731132




6,43731132










asked Nov 15 '18 at 2:27









dxdydzdxdydz

33110




33110








  • 1




    $begingroup$
    A great solution to method of characteristics for a system of PDEs is given here.
    $endgroup$
    – Mattos
    Nov 15 '18 at 3:47














  • 1




    $begingroup$
    A great solution to method of characteristics for a system of PDEs is given here.
    $endgroup$
    – Mattos
    Nov 15 '18 at 3:47








1




1




$begingroup$
A great solution to method of characteristics for a system of PDEs is given here.
$endgroup$
– Mattos
Nov 15 '18 at 3:47




$begingroup$
A great solution to method of characteristics for a system of PDEs is given here.
$endgroup$
– Mattos
Nov 15 '18 at 3:47










1 Answer
1






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2












$begingroup$

The system rewrites as ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$ with ${bf u} = (u,v)^top$. We diagonalize the matrix as ${bf M} = {bf S}, {bf J}, {bf S}^{-1}$ where $bf J$ is diagonal. Setting ${bf v} = {bf S}^{-1}{bf u}$, one obtains a diagonal system ${bf v}_t + {bf J}, {bf v}_x = {bf 0}$ which rows can be solved independently by using the method of characteristics. Then, $bf u$ is deduced from ${bf u} = {bf S},{bf v}$. Here, we find
begin{aligned}
u(x,t)&= frac{1}{2}big(u_0(x-t)+u_0(x+t)big)+frac{1}{2}big(v_0(x-t)-v_0(x+t)big)\
v(x,t)&= frac{1}{2}big(v_0(x-t)+v_0(x+t)big)+frac{1}{2}big(u_0(x-t)-u_0(x+t)big)
end{aligned}

This method works only for linear first-order systems ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$, which matrix $bf M$ can be diagonalized in $Bbb R$ (linear hyperbolic systems).






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    1 Answer
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    1 Answer
    1






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    oldest

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    active

    oldest

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    active

    oldest

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    2












    $begingroup$

    The system rewrites as ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$ with ${bf u} = (u,v)^top$. We diagonalize the matrix as ${bf M} = {bf S}, {bf J}, {bf S}^{-1}$ where $bf J$ is diagonal. Setting ${bf v} = {bf S}^{-1}{bf u}$, one obtains a diagonal system ${bf v}_t + {bf J}, {bf v}_x = {bf 0}$ which rows can be solved independently by using the method of characteristics. Then, $bf u$ is deduced from ${bf u} = {bf S},{bf v}$. Here, we find
    begin{aligned}
    u(x,t)&= frac{1}{2}big(u_0(x-t)+u_0(x+t)big)+frac{1}{2}big(v_0(x-t)-v_0(x+t)big)\
    v(x,t)&= frac{1}{2}big(v_0(x-t)+v_0(x+t)big)+frac{1}{2}big(u_0(x-t)-u_0(x+t)big)
    end{aligned}

    This method works only for linear first-order systems ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$, which matrix $bf M$ can be diagonalized in $Bbb R$ (linear hyperbolic systems).






    share|cite|improve this answer









    $endgroup$


















      2












      $begingroup$

      The system rewrites as ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$ with ${bf u} = (u,v)^top$. We diagonalize the matrix as ${bf M} = {bf S}, {bf J}, {bf S}^{-1}$ where $bf J$ is diagonal. Setting ${bf v} = {bf S}^{-1}{bf u}$, one obtains a diagonal system ${bf v}_t + {bf J}, {bf v}_x = {bf 0}$ which rows can be solved independently by using the method of characteristics. Then, $bf u$ is deduced from ${bf u} = {bf S},{bf v}$. Here, we find
      begin{aligned}
      u(x,t)&= frac{1}{2}big(u_0(x-t)+u_0(x+t)big)+frac{1}{2}big(v_0(x-t)-v_0(x+t)big)\
      v(x,t)&= frac{1}{2}big(v_0(x-t)+v_0(x+t)big)+frac{1}{2}big(u_0(x-t)-u_0(x+t)big)
      end{aligned}

      This method works only for linear first-order systems ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$, which matrix $bf M$ can be diagonalized in $Bbb R$ (linear hyperbolic systems).






      share|cite|improve this answer









      $endgroup$
















        2












        2








        2





        $begingroup$

        The system rewrites as ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$ with ${bf u} = (u,v)^top$. We diagonalize the matrix as ${bf M} = {bf S}, {bf J}, {bf S}^{-1}$ where $bf J$ is diagonal. Setting ${bf v} = {bf S}^{-1}{bf u}$, one obtains a diagonal system ${bf v}_t + {bf J}, {bf v}_x = {bf 0}$ which rows can be solved independently by using the method of characteristics. Then, $bf u$ is deduced from ${bf u} = {bf S},{bf v}$. Here, we find
        begin{aligned}
        u(x,t)&= frac{1}{2}big(u_0(x-t)+u_0(x+t)big)+frac{1}{2}big(v_0(x-t)-v_0(x+t)big)\
        v(x,t)&= frac{1}{2}big(v_0(x-t)+v_0(x+t)big)+frac{1}{2}big(u_0(x-t)-u_0(x+t)big)
        end{aligned}

        This method works only for linear first-order systems ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$, which matrix $bf M$ can be diagonalized in $Bbb R$ (linear hyperbolic systems).






        share|cite|improve this answer









        $endgroup$



        The system rewrites as ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$ with ${bf u} = (u,v)^top$. We diagonalize the matrix as ${bf M} = {bf S}, {bf J}, {bf S}^{-1}$ where $bf J$ is diagonal. Setting ${bf v} = {bf S}^{-1}{bf u}$, one obtains a diagonal system ${bf v}_t + {bf J}, {bf v}_x = {bf 0}$ which rows can be solved independently by using the method of characteristics. Then, $bf u$ is deduced from ${bf u} = {bf S},{bf v}$. Here, we find
        begin{aligned}
        u(x,t)&= frac{1}{2}big(u_0(x-t)+u_0(x+t)big)+frac{1}{2}big(v_0(x-t)-v_0(x+t)big)\
        v(x,t)&= frac{1}{2}big(v_0(x-t)+v_0(x+t)big)+frac{1}{2}big(u_0(x-t)-u_0(x+t)big)
        end{aligned}

        This method works only for linear first-order systems ${bf u}_t + {bf M}, {bf u}_x = {bf 0}$, which matrix $bf M$ can be diagonalized in $Bbb R$ (linear hyperbolic systems).







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Dec 9 '18 at 12:55









        Harry49Harry49

        6,43731132




        6,43731132






























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