Wave equation - use parallelogram rule to solve the problem Announcing the arrival of Valued Associate #679: Cesar Manara Planned maintenance scheduled April 23, 2019 at 00:00UTC (8:00pm US/Eastern)Problem related to wave equationSolve the following wave equationShow that the wave equation does not satisfy the maximum principleAnalyzing specific qualities of the Wave EquationSolution to wave equation case threeSolving the wave equation - d'Alembert's solutionCompatibility conditions for the wave equation with boundariesParallelogram property on Wave equationfind the value of $U(frac12,frac32)$ if satisfies the wave equationinhomogenous wave equation with initial value; PDE

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Wave equation - use parallelogram rule to solve the problem



Announcing the arrival of Valued Associate #679: Cesar Manara
Planned maintenance scheduled April 23, 2019 at 00:00UTC (8:00pm US/Eastern)Problem related to wave equationSolve the following wave equationShow that the wave equation does not satisfy the maximum principleAnalyzing specific qualities of the Wave EquationSolution to wave equation case threeSolving the wave equation - d'Alembert's solutionCompatibility conditions for the wave equation with boundariesParallelogram property on Wave equationfind the value of $U(frac12,frac32)$ if satisfies the wave equationinhomogenous wave equation with initial value; PDE










0












$begingroup$


Given wave equation: $ u_tt-c^2u_xx=0 $, let u be a solution.



Points A, B, C, D are vertices of parallelogram of two pairs of characteristic lines: $ x-ct=c1, x-ct=c2, x+ct=d1, x+ct=d2 $



Use parallelogram rule to find u that satisfies this:



$ u_tt-u_xx=0, u(-a,a)=a,$ $ $ $ u(a,a)=a^2 $ for $ a>0 $



Guys, how can I use parallelogram rule here? I know that if we draw the characteristic lines we will get picture like that.
parallelogram based on vertices of characteristic lines










share|cite|improve this question









$endgroup$
















    0












    $begingroup$


    Given wave equation: $ u_tt-c^2u_xx=0 $, let u be a solution.



    Points A, B, C, D are vertices of parallelogram of two pairs of characteristic lines: $ x-ct=c1, x-ct=c2, x+ct=d1, x+ct=d2 $



    Use parallelogram rule to find u that satisfies this:



    $ u_tt-u_xx=0, u(-a,a)=a,$ $ $ $ u(a,a)=a^2 $ for $ a>0 $



    Guys, how can I use parallelogram rule here? I know that if we draw the characteristic lines we will get picture like that.
    parallelogram based on vertices of characteristic lines










    share|cite|improve this question









    $endgroup$














      0












      0








      0


      1



      $begingroup$


      Given wave equation: $ u_tt-c^2u_xx=0 $, let u be a solution.



      Points A, B, C, D are vertices of parallelogram of two pairs of characteristic lines: $ x-ct=c1, x-ct=c2, x+ct=d1, x+ct=d2 $



      Use parallelogram rule to find u that satisfies this:



      $ u_tt-u_xx=0, u(-a,a)=a,$ $ $ $ u(a,a)=a^2 $ for $ a>0 $



      Guys, how can I use parallelogram rule here? I know that if we draw the characteristic lines we will get picture like that.
      parallelogram based on vertices of characteristic lines










      share|cite|improve this question









      $endgroup$




      Given wave equation: $ u_tt-c^2u_xx=0 $, let u be a solution.



      Points A, B, C, D are vertices of parallelogram of two pairs of characteristic lines: $ x-ct=c1, x-ct=c2, x+ct=d1, x+ct=d2 $



      Use parallelogram rule to find u that satisfies this:



      $ u_tt-u_xx=0, u(-a,a)=a,$ $ $ $ u(a,a)=a^2 $ for $ a>0 $



      Guys, how can I use parallelogram rule here? I know that if we draw the characteristic lines we will get picture like that.
      parallelogram based on vertices of characteristic lines







      pde wave-equation






      share|cite|improve this question













      share|cite|improve this question











      share|cite|improve this question




      share|cite|improve this question










      asked Mar 27 at 20:29









      Alpys RauanAlpys Rauan

      111




      111




















          1 Answer
          1






          active

          oldest

          votes


















          0












          $begingroup$

          You are given data on the "angle" $y=-x,, xle 0$ and $y=x,, xge 0$. If you take any point $P(x_0,y_0)$ inside this angle (above the given lines) and you draw characteristic lines parallel to the sides of the angle, the value of $u$ there is the sum of the values carried by the characteristics (this is what the general solution of the wave equation is). The intersections with the sides of the angle are $(fracx_0+y_02, fracx_0+y_02)$ (characteristic with slope $-1$) and $(fracx_0-y_02, fracy_0-x_02)$ (characteristic with slope $+1$). Then,
          $$
          u(x_0,y_0)=fracy_0-x_02+left(fracx_0+y_02right)^2
          $$

          The solution is not determined uniquely outside of the angle.



          The parallelogram rule just tells you that the sums of the values of the solution at opposite vertices of a parallelogram are equal. In your case the parallelogram is formed by $(x_0,y_0)$, $(0,0)$ and the intersections of the characteristics with the initial angle I mentioned before. You get the same answer of course.



          Hope this helps.






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            Dear GReyes, can you explain how did you find that equation about ?
            $endgroup$
            – Alpys Rauan
            Mar 29 at 12:49










          • $begingroup$
            The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
            $endgroup$
            – GReyes
            Mar 30 at 16:21











          Your Answer








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          1 Answer
          1






          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          0












          $begingroup$

          You are given data on the "angle" $y=-x,, xle 0$ and $y=x,, xge 0$. If you take any point $P(x_0,y_0)$ inside this angle (above the given lines) and you draw characteristic lines parallel to the sides of the angle, the value of $u$ there is the sum of the values carried by the characteristics (this is what the general solution of the wave equation is). The intersections with the sides of the angle are $(fracx_0+y_02, fracx_0+y_02)$ (characteristic with slope $-1$) and $(fracx_0-y_02, fracy_0-x_02)$ (characteristic with slope $+1$). Then,
          $$
          u(x_0,y_0)=fracy_0-x_02+left(fracx_0+y_02right)^2
          $$

          The solution is not determined uniquely outside of the angle.



          The parallelogram rule just tells you that the sums of the values of the solution at opposite vertices of a parallelogram are equal. In your case the parallelogram is formed by $(x_0,y_0)$, $(0,0)$ and the intersections of the characteristics with the initial angle I mentioned before. You get the same answer of course.



          Hope this helps.






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            Dear GReyes, can you explain how did you find that equation about ?
            $endgroup$
            – Alpys Rauan
            Mar 29 at 12:49










          • $begingroup$
            The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
            $endgroup$
            – GReyes
            Mar 30 at 16:21















          0












          $begingroup$

          You are given data on the "angle" $y=-x,, xle 0$ and $y=x,, xge 0$. If you take any point $P(x_0,y_0)$ inside this angle (above the given lines) and you draw characteristic lines parallel to the sides of the angle, the value of $u$ there is the sum of the values carried by the characteristics (this is what the general solution of the wave equation is). The intersections with the sides of the angle are $(fracx_0+y_02, fracx_0+y_02)$ (characteristic with slope $-1$) and $(fracx_0-y_02, fracy_0-x_02)$ (characteristic with slope $+1$). Then,
          $$
          u(x_0,y_0)=fracy_0-x_02+left(fracx_0+y_02right)^2
          $$

          The solution is not determined uniquely outside of the angle.



          The parallelogram rule just tells you that the sums of the values of the solution at opposite vertices of a parallelogram are equal. In your case the parallelogram is formed by $(x_0,y_0)$, $(0,0)$ and the intersections of the characteristics with the initial angle I mentioned before. You get the same answer of course.



          Hope this helps.






          share|cite|improve this answer











          $endgroup$












          • $begingroup$
            Dear GReyes, can you explain how did you find that equation about ?
            $endgroup$
            – Alpys Rauan
            Mar 29 at 12:49










          • $begingroup$
            The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
            $endgroup$
            – GReyes
            Mar 30 at 16:21













          0












          0








          0





          $begingroup$

          You are given data on the "angle" $y=-x,, xle 0$ and $y=x,, xge 0$. If you take any point $P(x_0,y_0)$ inside this angle (above the given lines) and you draw characteristic lines parallel to the sides of the angle, the value of $u$ there is the sum of the values carried by the characteristics (this is what the general solution of the wave equation is). The intersections with the sides of the angle are $(fracx_0+y_02, fracx_0+y_02)$ (characteristic with slope $-1$) and $(fracx_0-y_02, fracy_0-x_02)$ (characteristic with slope $+1$). Then,
          $$
          u(x_0,y_0)=fracy_0-x_02+left(fracx_0+y_02right)^2
          $$

          The solution is not determined uniquely outside of the angle.



          The parallelogram rule just tells you that the sums of the values of the solution at opposite vertices of a parallelogram are equal. In your case the parallelogram is formed by $(x_0,y_0)$, $(0,0)$ and the intersections of the characteristics with the initial angle I mentioned before. You get the same answer of course.



          Hope this helps.






          share|cite|improve this answer











          $endgroup$



          You are given data on the "angle" $y=-x,, xle 0$ and $y=x,, xge 0$. If you take any point $P(x_0,y_0)$ inside this angle (above the given lines) and you draw characteristic lines parallel to the sides of the angle, the value of $u$ there is the sum of the values carried by the characteristics (this is what the general solution of the wave equation is). The intersections with the sides of the angle are $(fracx_0+y_02, fracx_0+y_02)$ (characteristic with slope $-1$) and $(fracx_0-y_02, fracy_0-x_02)$ (characteristic with slope $+1$). Then,
          $$
          u(x_0,y_0)=fracy_0-x_02+left(fracx_0+y_02right)^2
          $$

          The solution is not determined uniquely outside of the angle.



          The parallelogram rule just tells you that the sums of the values of the solution at opposite vertices of a parallelogram are equal. In your case the parallelogram is formed by $(x_0,y_0)$, $(0,0)$ and the intersections of the characteristics with the initial angle I mentioned before. You get the same answer of course.



          Hope this helps.







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Mar 28 at 2:59

























          answered Mar 27 at 23:09









          GReyesGReyes

          2,57315




          2,57315











          • $begingroup$
            Dear GReyes, can you explain how did you find that equation about ?
            $endgroup$
            – Alpys Rauan
            Mar 29 at 12:49










          • $begingroup$
            The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
            $endgroup$
            – GReyes
            Mar 30 at 16:21
















          • $begingroup$
            Dear GReyes, can you explain how did you find that equation about ?
            $endgroup$
            – Alpys Rauan
            Mar 29 at 12:49










          • $begingroup$
            The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
            $endgroup$
            – GReyes
            Mar 30 at 16:21















          $begingroup$
          Dear GReyes, can you explain how did you find that equation about ?
          $endgroup$
          – Alpys Rauan
          Mar 29 at 12:49




          $begingroup$
          Dear GReyes, can you explain how did you find that equation about ?
          $endgroup$
          – Alpys Rauan
          Mar 29 at 12:49












          $begingroup$
          The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
          $endgroup$
          – GReyes
          Mar 30 at 16:21




          $begingroup$
          The parallelogram rule is a direct consequence of the form of the general solution $u(x,t)=F(x+ct)+G(x-ct)$ of the wave equation $u_tt=c^2u_xx$. If you form a parallelogram in the $(x,t)$-plane with vertices $A,B,C,D$ (say, in that order clockwise) with slopes $+c$ and $-c$, then $u(A)+u(C)=u(B)+u(D)$. This is a straightforward consequence of the fact that $F$ is a constant along two of the opposite sides and $G$ is constant along the other two. You choose your vertices $A(0,0)$, $C(x_0,y_0)$, and $B$ and $D$ are the intersections of the characteristics with your initial angle.
          $endgroup$
          – GReyes
          Mar 30 at 16:21

















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