Solve: $xu_x+(x+y)u_y=1$











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Solve the following PDE



$$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane




$$begin{cases}
a=x\
b=x+y\
c=1
end{cases}Rightarrow begin{cases}
frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
frac{du}{dt}=1iff du=dtiff u=t+c_2
end{cases}$$



How do I solve $?_1$ and what should be my next step?










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    Solve the following PDE



    $$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane




    $$begin{cases}
    a=x\
    b=x+y\
    c=1
    end{cases}Rightarrow begin{cases}
    frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
    frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
    frac{du}{dt}=1iff du=dtiff u=t+c_2
    end{cases}$$



    How do I solve $?_1$ and what should be my next step?










    share|cite|improve this question


























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      Solve the following PDE



      $$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane




      $$begin{cases}
      a=x\
      b=x+y\
      c=1
      end{cases}Rightarrow begin{cases}
      frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
      frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
      frac{du}{dt}=1iff du=dtiff u=t+c_2
      end{cases}$$



      How do I solve $?_1$ and what should be my next step?










      share|cite|improve this question
















      Solve the following PDE



      $$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane




      $$begin{cases}
      a=x\
      b=x+y\
      c=1
      end{cases}Rightarrow begin{cases}
      frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
      frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
      frac{du}{dt}=1iff du=dtiff u=t+c_2
      end{cases}$$



      How do I solve $?_1$ and what should be my next step?







      differential-equations pde






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      edited Nov 15 at 17:13

























      asked Nov 15 at 16:27









      newhere

      838311




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          2 Answers
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          $$xu_x+(x+y)u_y=1$$
          You have got the correct system of equation which can be written on this form :
          $$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
          Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
          $$frac{y}{x}-ln|x|=c_1$$
          Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
          $$u-ln|x|=c_2$$
          The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
          $$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
          where $F$ is an arbitrary function.



          This function is determined according to the boundary condition :



          $u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$



          Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .



          $u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$



          The final solution is :
          $$u(x,y)=frac{y}{x}$$






          share|cite|improve this answer























          • + Hi JJacquelin i was just solving it I ended with the same answer..
            – Isham
            Nov 15 at 18:18










          • The method you used is Lagrange method?
            – newhere
            Nov 15 at 22:55










          • In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
            – JJacquelin
            Nov 16 at 7:12


















          up vote
          1
          down vote













          The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
          $$
          frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
          $$






          share|cite|improve this answer





















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            2 Answers
            2






            active

            oldest

            votes








            2 Answers
            2






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes








            up vote
            2
            down vote













            $$xu_x+(x+y)u_y=1$$
            You have got the correct system of equation which can be written on this form :
            $$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
            Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
            $$frac{y}{x}-ln|x|=c_1$$
            Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
            $$u-ln|x|=c_2$$
            The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
            $$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
            where $F$ is an arbitrary function.



            This function is determined according to the boundary condition :



            $u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$



            Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .



            $u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$



            The final solution is :
            $$u(x,y)=frac{y}{x}$$






            share|cite|improve this answer























            • + Hi JJacquelin i was just solving it I ended with the same answer..
              – Isham
              Nov 15 at 18:18










            • The method you used is Lagrange method?
              – newhere
              Nov 15 at 22:55










            • In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
              – JJacquelin
              Nov 16 at 7:12















            up vote
            2
            down vote













            $$xu_x+(x+y)u_y=1$$
            You have got the correct system of equation which can be written on this form :
            $$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
            Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
            $$frac{y}{x}-ln|x|=c_1$$
            Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
            $$u-ln|x|=c_2$$
            The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
            $$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
            where $F$ is an arbitrary function.



            This function is determined according to the boundary condition :



            $u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$



            Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .



            $u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$



            The final solution is :
            $$u(x,y)=frac{y}{x}$$






            share|cite|improve this answer























            • + Hi JJacquelin i was just solving it I ended with the same answer..
              – Isham
              Nov 15 at 18:18










            • The method you used is Lagrange method?
              – newhere
              Nov 15 at 22:55










            • In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
              – JJacquelin
              Nov 16 at 7:12













            up vote
            2
            down vote










            up vote
            2
            down vote









            $$xu_x+(x+y)u_y=1$$
            You have got the correct system of equation which can be written on this form :
            $$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
            Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
            $$frac{y}{x}-ln|x|=c_1$$
            Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
            $$u-ln|x|=c_2$$
            The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
            $$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
            where $F$ is an arbitrary function.



            This function is determined according to the boundary condition :



            $u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$



            Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .



            $u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$



            The final solution is :
            $$u(x,y)=frac{y}{x}$$






            share|cite|improve this answer














            $$xu_x+(x+y)u_y=1$$
            You have got the correct system of equation which can be written on this form :
            $$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
            Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
            $$frac{y}{x}-ln|x|=c_1$$
            Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
            $$u-ln|x|=c_2$$
            The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
            $$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
            where $F$ is an arbitrary function.



            This function is determined according to the boundary condition :



            $u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$



            Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .



            $u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$



            The final solution is :
            $$u(x,y)=frac{y}{x}$$







            share|cite|improve this answer














            share|cite|improve this answer



            share|cite|improve this answer








            edited Nov 15 at 18:20

























            answered Nov 15 at 18:16









            JJacquelin

            42k21750




            42k21750












            • + Hi JJacquelin i was just solving it I ended with the same answer..
              – Isham
              Nov 15 at 18:18










            • The method you used is Lagrange method?
              – newhere
              Nov 15 at 22:55










            • In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
              – JJacquelin
              Nov 16 at 7:12


















            • + Hi JJacquelin i was just solving it I ended with the same answer..
              – Isham
              Nov 15 at 18:18










            • The method you used is Lagrange method?
              – newhere
              Nov 15 at 22:55










            • In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
              – JJacquelin
              Nov 16 at 7:12
















            + Hi JJacquelin i was just solving it I ended with the same answer..
            – Isham
            Nov 15 at 18:18




            + Hi JJacquelin i was just solving it I ended with the same answer..
            – Isham
            Nov 15 at 18:18












            The method you used is Lagrange method?
            – newhere
            Nov 15 at 22:55




            The method you used is Lagrange method?
            – newhere
            Nov 15 at 22:55












            In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
            – JJacquelin
            Nov 16 at 7:12




            In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
            – JJacquelin
            Nov 16 at 7:12










            up vote
            1
            down vote













            The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
            $$
            frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
            $$






            share|cite|improve this answer

























              up vote
              1
              down vote













              The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
              $$
              frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
              $$






              share|cite|improve this answer























                up vote
                1
                down vote










                up vote
                1
                down vote









                The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
                $$
                frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
                $$






                share|cite|improve this answer












                The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
                $$
                frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
                $$







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Nov 15 at 16:40









                LutzL

                53.7k41953




                53.7k41953






























                     

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