Second order partial Cauchy problem with two functions












2












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I have the following Cauchy problem. I do not know where to start, so I would appreciate any help and tips.
$$frac{partial^2 Y(t, x)}{partial t^2} = 9frac{partial^2 Y(t,x)}{partial x^2} - 2Z(t,x)$$
$$frac{partial^2 Z(t, x)}{partial t^2} = 6frac{partial^2 Z(t,x)}{partial x^2} - 2Y(t,x)$$
$$Y(0, x) = cos(x), Z(0, x) = 0$$
$$frac{partial Y(t, 0)}{partial t} = frac{partial Z(t, 0)}{partial t} = 0$$










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  • $begingroup$
    It is a partial derivative wrt $t$ in the last eqution, isn’t it?
    $endgroup$
    – Mindlack
    Dec 12 '18 at 15:51










  • $begingroup$
    yes you are right
    $endgroup$
    – Akari Gale
    Dec 12 '18 at 16:02










  • $begingroup$
    Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
    $endgroup$
    – Mindlack
    Dec 12 '18 at 16:17










  • $begingroup$
    An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
    $endgroup$
    – whpowell96
    Dec 12 '18 at 19:31












  • $begingroup$
    If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
    $endgroup$
    – Yuri Negometyanov
    Dec 13 '18 at 9:27
















2












$begingroup$


I have the following Cauchy problem. I do not know where to start, so I would appreciate any help and tips.
$$frac{partial^2 Y(t, x)}{partial t^2} = 9frac{partial^2 Y(t,x)}{partial x^2} - 2Z(t,x)$$
$$frac{partial^2 Z(t, x)}{partial t^2} = 6frac{partial^2 Z(t,x)}{partial x^2} - 2Y(t,x)$$
$$Y(0, x) = cos(x), Z(0, x) = 0$$
$$frac{partial Y(t, 0)}{partial t} = frac{partial Z(t, 0)}{partial t} = 0$$










share|cite|improve this question











$endgroup$












  • $begingroup$
    It is a partial derivative wrt $t$ in the last eqution, isn’t it?
    $endgroup$
    – Mindlack
    Dec 12 '18 at 15:51










  • $begingroup$
    yes you are right
    $endgroup$
    – Akari Gale
    Dec 12 '18 at 16:02










  • $begingroup$
    Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
    $endgroup$
    – Mindlack
    Dec 12 '18 at 16:17










  • $begingroup$
    An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
    $endgroup$
    – whpowell96
    Dec 12 '18 at 19:31












  • $begingroup$
    If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
    $endgroup$
    – Yuri Negometyanov
    Dec 13 '18 at 9:27














2












2








2





$begingroup$


I have the following Cauchy problem. I do not know where to start, so I would appreciate any help and tips.
$$frac{partial^2 Y(t, x)}{partial t^2} = 9frac{partial^2 Y(t,x)}{partial x^2} - 2Z(t,x)$$
$$frac{partial^2 Z(t, x)}{partial t^2} = 6frac{partial^2 Z(t,x)}{partial x^2} - 2Y(t,x)$$
$$Y(0, x) = cos(x), Z(0, x) = 0$$
$$frac{partial Y(t, 0)}{partial t} = frac{partial Z(t, 0)}{partial t} = 0$$










share|cite|improve this question











$endgroup$




I have the following Cauchy problem. I do not know where to start, so I would appreciate any help and tips.
$$frac{partial^2 Y(t, x)}{partial t^2} = 9frac{partial^2 Y(t,x)}{partial x^2} - 2Z(t,x)$$
$$frac{partial^2 Z(t, x)}{partial t^2} = 6frac{partial^2 Z(t,x)}{partial x^2} - 2Y(t,x)$$
$$Y(0, x) = cos(x), Z(0, x) = 0$$
$$frac{partial Y(t, 0)}{partial t} = frac{partial Z(t, 0)}{partial t} = 0$$







ordinary-differential-equations pde






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edited Dec 12 '18 at 22:11









Alex Ravsky

40.4k32282




40.4k32282










asked Dec 9 '18 at 20:30









Akari GaleAkari Gale

1096




1096












  • $begingroup$
    It is a partial derivative wrt $t$ in the last eqution, isn’t it?
    $endgroup$
    – Mindlack
    Dec 12 '18 at 15:51










  • $begingroup$
    yes you are right
    $endgroup$
    – Akari Gale
    Dec 12 '18 at 16:02










  • $begingroup$
    Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
    $endgroup$
    – Mindlack
    Dec 12 '18 at 16:17










  • $begingroup$
    An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
    $endgroup$
    – whpowell96
    Dec 12 '18 at 19:31












  • $begingroup$
    If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
    $endgroup$
    – Yuri Negometyanov
    Dec 13 '18 at 9:27


















  • $begingroup$
    It is a partial derivative wrt $t$ in the last eqution, isn’t it?
    $endgroup$
    – Mindlack
    Dec 12 '18 at 15:51










  • $begingroup$
    yes you are right
    $endgroup$
    – Akari Gale
    Dec 12 '18 at 16:02










  • $begingroup$
    Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
    $endgroup$
    – Mindlack
    Dec 12 '18 at 16:17










  • $begingroup$
    An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
    $endgroup$
    – whpowell96
    Dec 12 '18 at 19:31












  • $begingroup$
    If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
    $endgroup$
    – Yuri Negometyanov
    Dec 13 '18 at 9:27
















$begingroup$
It is a partial derivative wrt $t$ in the last eqution, isn’t it?
$endgroup$
– Mindlack
Dec 12 '18 at 15:51




$begingroup$
It is a partial derivative wrt $t$ in the last eqution, isn’t it?
$endgroup$
– Mindlack
Dec 12 '18 at 15:51












$begingroup$
yes you are right
$endgroup$
– Akari Gale
Dec 12 '18 at 16:02




$begingroup$
yes you are right
$endgroup$
– Akari Gale
Dec 12 '18 at 16:02












$begingroup$
Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
$endgroup$
– Mindlack
Dec 12 '18 at 16:17




$begingroup$
Do you really have $Z(t,0)=0$ for each $t$? Another thing: this is not a Cauchy problem, it is a PDE and this kind of problem is usually much harder.
$endgroup$
– Mindlack
Dec 12 '18 at 16:17












$begingroup$
An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
$endgroup$
– whpowell96
Dec 12 '18 at 19:31






$begingroup$
An IVP for a PDE over all of $mathbb{R}$ is usually called a Cauchy Problem
$endgroup$
– whpowell96
Dec 12 '18 at 19:31














$begingroup$
If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
$endgroup$
– Yuri Negometyanov
Dec 13 '18 at 9:27




$begingroup$
If the first equation did not contain $Z,$ and the second one did not contain $Y,$, then each of them would require four conditions. This means that four more conditions are needed.
$endgroup$
– Yuri Negometyanov
Dec 13 '18 at 9:27










2 Answers
2






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oldest

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1












$begingroup$

Your equation is linear, so you could try expanding the solutions in a Fourier series. Moreover, as the initial condition is given in terms of $cos(x)$, it's a good idea to write
begin{align}
Y(t,x) &= sum_{k=0}^infty a_Y(k,t) cos(k x) + b_Y(k,t) sin(k x)\
Z(t,x) &= sum_{k=0}^infty a_Z(k,t) cos(k x) + b_Z(k,t) sin(k x)
end{align}

which yields a linear system of ordinary differential equations for the coefficients $a_{Y,Z}(k,t)$ and $b_{Y,Z}(k,t)$. The initial conditions of the PDE system then translate in
begin{equation}
a_Y(1,0) = 1,quad a_Y(k,0) = 0 ; (k neq 1),quad b_Y(k,0) = 0 = b_Z(k,0),
end{equation}

which are initial conditions for the ODE system. The boundary condition(s) translate in
begin{equation}
frac{partial Y}{partial t}(t,0) = sum_{k=0}^infty frac{text{d} a_Y}{text{d} t}(k,t) = 0 = sum_{k=0}^infty frac{text{d} a_Z}{text{d} t}(k,t) = frac{partial Z}{partial t}(t,0).
end{equation}

Note that, as it stands, the initial- and boundary conditions do not fully determine the solution.






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    $$begin{cases}
    2Y(t,x) = 6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}\[4px]
    2dfrac{partial^2 Y(t, x)}{partial t^2} = 18dfrac{partial^2 Y(t,x)}{partial x^2} - 4Z(t,x),
    end{cases}$$

    so
    $$dfrac{partial^2}{partial t^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) = 9dfrac{partial^2}{partial x^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) - 4Z(t,x),$$
    $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
    Z(0, x) = 0\[4pt]
    6dfrac{partial^2 Z(0,x)}{partial x^2} - dfrac{partial^2 Z(0, x)}{partial t^2} = 2cos(x)\[4pt]
    6dfrac{partial^3 Z(t,0)}{partial tpartial x^2} - dfrac{partial^3 Z(t, 0)}{partial t^3} = 0\[4pt]
    dfrac{partial Z(t, 0)}{partial t} = 0
    end{cases}$$



    $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
    Z(0, x) = 0,quad dfrac{partial^2 Z(0,x)}{partial x^2} = dfrac13cos(x)\[4pt]
    dfrac{partial Z(t, 0)}{partial t} = 0,quaddfrac{partial^3 Z(t, 0)}{partial t^3} = 0.
    end{cases}$$

    And it reqires four conditions more.






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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      1












      $begingroup$

      Your equation is linear, so you could try expanding the solutions in a Fourier series. Moreover, as the initial condition is given in terms of $cos(x)$, it's a good idea to write
      begin{align}
      Y(t,x) &= sum_{k=0}^infty a_Y(k,t) cos(k x) + b_Y(k,t) sin(k x)\
      Z(t,x) &= sum_{k=0}^infty a_Z(k,t) cos(k x) + b_Z(k,t) sin(k x)
      end{align}

      which yields a linear system of ordinary differential equations for the coefficients $a_{Y,Z}(k,t)$ and $b_{Y,Z}(k,t)$. The initial conditions of the PDE system then translate in
      begin{equation}
      a_Y(1,0) = 1,quad a_Y(k,0) = 0 ; (k neq 1),quad b_Y(k,0) = 0 = b_Z(k,0),
      end{equation}

      which are initial conditions for the ODE system. The boundary condition(s) translate in
      begin{equation}
      frac{partial Y}{partial t}(t,0) = sum_{k=0}^infty frac{text{d} a_Y}{text{d} t}(k,t) = 0 = sum_{k=0}^infty frac{text{d} a_Z}{text{d} t}(k,t) = frac{partial Z}{partial t}(t,0).
      end{equation}

      Note that, as it stands, the initial- and boundary conditions do not fully determine the solution.






      share|cite|improve this answer









      $endgroup$


















        1












        $begingroup$

        Your equation is linear, so you could try expanding the solutions in a Fourier series. Moreover, as the initial condition is given in terms of $cos(x)$, it's a good idea to write
        begin{align}
        Y(t,x) &= sum_{k=0}^infty a_Y(k,t) cos(k x) + b_Y(k,t) sin(k x)\
        Z(t,x) &= sum_{k=0}^infty a_Z(k,t) cos(k x) + b_Z(k,t) sin(k x)
        end{align}

        which yields a linear system of ordinary differential equations for the coefficients $a_{Y,Z}(k,t)$ and $b_{Y,Z}(k,t)$. The initial conditions of the PDE system then translate in
        begin{equation}
        a_Y(1,0) = 1,quad a_Y(k,0) = 0 ; (k neq 1),quad b_Y(k,0) = 0 = b_Z(k,0),
        end{equation}

        which are initial conditions for the ODE system. The boundary condition(s) translate in
        begin{equation}
        frac{partial Y}{partial t}(t,0) = sum_{k=0}^infty frac{text{d} a_Y}{text{d} t}(k,t) = 0 = sum_{k=0}^infty frac{text{d} a_Z}{text{d} t}(k,t) = frac{partial Z}{partial t}(t,0).
        end{equation}

        Note that, as it stands, the initial- and boundary conditions do not fully determine the solution.






        share|cite|improve this answer









        $endgroup$
















          1












          1








          1





          $begingroup$

          Your equation is linear, so you could try expanding the solutions in a Fourier series. Moreover, as the initial condition is given in terms of $cos(x)$, it's a good idea to write
          begin{align}
          Y(t,x) &= sum_{k=0}^infty a_Y(k,t) cos(k x) + b_Y(k,t) sin(k x)\
          Z(t,x) &= sum_{k=0}^infty a_Z(k,t) cos(k x) + b_Z(k,t) sin(k x)
          end{align}

          which yields a linear system of ordinary differential equations for the coefficients $a_{Y,Z}(k,t)$ and $b_{Y,Z}(k,t)$. The initial conditions of the PDE system then translate in
          begin{equation}
          a_Y(1,0) = 1,quad a_Y(k,0) = 0 ; (k neq 1),quad b_Y(k,0) = 0 = b_Z(k,0),
          end{equation}

          which are initial conditions for the ODE system. The boundary condition(s) translate in
          begin{equation}
          frac{partial Y}{partial t}(t,0) = sum_{k=0}^infty frac{text{d} a_Y}{text{d} t}(k,t) = 0 = sum_{k=0}^infty frac{text{d} a_Z}{text{d} t}(k,t) = frac{partial Z}{partial t}(t,0).
          end{equation}

          Note that, as it stands, the initial- and boundary conditions do not fully determine the solution.






          share|cite|improve this answer









          $endgroup$



          Your equation is linear, so you could try expanding the solutions in a Fourier series. Moreover, as the initial condition is given in terms of $cos(x)$, it's a good idea to write
          begin{align}
          Y(t,x) &= sum_{k=0}^infty a_Y(k,t) cos(k x) + b_Y(k,t) sin(k x)\
          Z(t,x) &= sum_{k=0}^infty a_Z(k,t) cos(k x) + b_Z(k,t) sin(k x)
          end{align}

          which yields a linear system of ordinary differential equations for the coefficients $a_{Y,Z}(k,t)$ and $b_{Y,Z}(k,t)$. The initial conditions of the PDE system then translate in
          begin{equation}
          a_Y(1,0) = 1,quad a_Y(k,0) = 0 ; (k neq 1),quad b_Y(k,0) = 0 = b_Z(k,0),
          end{equation}

          which are initial conditions for the ODE system. The boundary condition(s) translate in
          begin{equation}
          frac{partial Y}{partial t}(t,0) = sum_{k=0}^infty frac{text{d} a_Y}{text{d} t}(k,t) = 0 = sum_{k=0}^infty frac{text{d} a_Z}{text{d} t}(k,t) = frac{partial Z}{partial t}(t,0).
          end{equation}

          Note that, as it stands, the initial- and boundary conditions do not fully determine the solution.







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          share|cite|improve this answer



          share|cite|improve this answer










          answered Dec 17 '18 at 14:18









          Frits VeermanFrits Veerman

          6,5362920




          6,5362920























              0












              $begingroup$

              $$begin{cases}
              2Y(t,x) = 6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}\[4px]
              2dfrac{partial^2 Y(t, x)}{partial t^2} = 18dfrac{partial^2 Y(t,x)}{partial x^2} - 4Z(t,x),
              end{cases}$$

              so
              $$dfrac{partial^2}{partial t^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) = 9dfrac{partial^2}{partial x^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) - 4Z(t,x),$$
              $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
              Z(0, x) = 0\[4pt]
              6dfrac{partial^2 Z(0,x)}{partial x^2} - dfrac{partial^2 Z(0, x)}{partial t^2} = 2cos(x)\[4pt]
              6dfrac{partial^3 Z(t,0)}{partial tpartial x^2} - dfrac{partial^3 Z(t, 0)}{partial t^3} = 0\[4pt]
              dfrac{partial Z(t, 0)}{partial t} = 0
              end{cases}$$



              $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
              Z(0, x) = 0,quad dfrac{partial^2 Z(0,x)}{partial x^2} = dfrac13cos(x)\[4pt]
              dfrac{partial Z(t, 0)}{partial t} = 0,quaddfrac{partial^3 Z(t, 0)}{partial t^3} = 0.
              end{cases}$$

              And it reqires four conditions more.






              share|cite|improve this answer









              $endgroup$


















                0












                $begingroup$

                $$begin{cases}
                2Y(t,x) = 6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}\[4px]
                2dfrac{partial^2 Y(t, x)}{partial t^2} = 18dfrac{partial^2 Y(t,x)}{partial x^2} - 4Z(t,x),
                end{cases}$$

                so
                $$dfrac{partial^2}{partial t^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) = 9dfrac{partial^2}{partial x^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) - 4Z(t,x),$$
                $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                Z(0, x) = 0\[4pt]
                6dfrac{partial^2 Z(0,x)}{partial x^2} - dfrac{partial^2 Z(0, x)}{partial t^2} = 2cos(x)\[4pt]
                6dfrac{partial^3 Z(t,0)}{partial tpartial x^2} - dfrac{partial^3 Z(t, 0)}{partial t^3} = 0\[4pt]
                dfrac{partial Z(t, 0)}{partial t} = 0
                end{cases}$$



                $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                Z(0, x) = 0,quad dfrac{partial^2 Z(0,x)}{partial x^2} = dfrac13cos(x)\[4pt]
                dfrac{partial Z(t, 0)}{partial t} = 0,quaddfrac{partial^3 Z(t, 0)}{partial t^3} = 0.
                end{cases}$$

                And it reqires four conditions more.






                share|cite|improve this answer









                $endgroup$
















                  0












                  0








                  0





                  $begingroup$

                  $$begin{cases}
                  2Y(t,x) = 6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}\[4px]
                  2dfrac{partial^2 Y(t, x)}{partial t^2} = 18dfrac{partial^2 Y(t,x)}{partial x^2} - 4Z(t,x),
                  end{cases}$$

                  so
                  $$dfrac{partial^2}{partial t^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) = 9dfrac{partial^2}{partial x^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) - 4Z(t,x),$$
                  $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                  Z(0, x) = 0\[4pt]
                  6dfrac{partial^2 Z(0,x)}{partial x^2} - dfrac{partial^2 Z(0, x)}{partial t^2} = 2cos(x)\[4pt]
                  6dfrac{partial^3 Z(t,0)}{partial tpartial x^2} - dfrac{partial^3 Z(t, 0)}{partial t^3} = 0\[4pt]
                  dfrac{partial Z(t, 0)}{partial t} = 0
                  end{cases}$$



                  $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                  Z(0, x) = 0,quad dfrac{partial^2 Z(0,x)}{partial x^2} = dfrac13cos(x)\[4pt]
                  dfrac{partial Z(t, 0)}{partial t} = 0,quaddfrac{partial^3 Z(t, 0)}{partial t^3} = 0.
                  end{cases}$$

                  And it reqires four conditions more.






                  share|cite|improve this answer









                  $endgroup$



                  $$begin{cases}
                  2Y(t,x) = 6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}\[4px]
                  2dfrac{partial^2 Y(t, x)}{partial t^2} = 18dfrac{partial^2 Y(t,x)}{partial x^2} - 4Z(t,x),
                  end{cases}$$

                  so
                  $$dfrac{partial^2}{partial t^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) = 9dfrac{partial^2}{partial x^2}left(6dfrac{partial^2 Z(t,x)}{partial x^2} - dfrac{partial^2 Z(t, x)}{partial t^2}right) - 4Z(t,x),$$
                  $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                  Z(0, x) = 0\[4pt]
                  6dfrac{partial^2 Z(0,x)}{partial x^2} - dfrac{partial^2 Z(0, x)}{partial t^2} = 2cos(x)\[4pt]
                  6dfrac{partial^3 Z(t,0)}{partial tpartial x^2} - dfrac{partial^3 Z(t, 0)}{partial t^3} = 0\[4pt]
                  dfrac{partial Z(t, 0)}{partial t} = 0
                  end{cases}$$



                  $$begin{cases}dfrac{partial^4 Z(t,x)}{partial t^4} - 15dfrac{partial^4 Z(t,x)}{partial t^2partial x^2} + 54dfrac{partial^4 Z(t,x)}{partial x^4}-4Z(t,x) = 0\[4pt]
                  Z(0, x) = 0,quad dfrac{partial^2 Z(0,x)}{partial x^2} = dfrac13cos(x)\[4pt]
                  dfrac{partial Z(t, 0)}{partial t} = 0,quaddfrac{partial^3 Z(t, 0)}{partial t^3} = 0.
                  end{cases}$$

                  And it reqires four conditions more.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Dec 15 '18 at 16:58









                  Yuri NegometyanovYuri Negometyanov

                  11.2k1728




                  11.2k1728






























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