General solution vs General Integral












1












$begingroup$


I have been reading some notes about Quasi Linear PDE and I stuck to the following issue:



Consider the PDE: $xz_x+yz_y=xe^{-z}$



then my notes read as:




"the general solution is: $G(x/y, e^z-x)=0$ . (1)



and so $$e^z-x=g(x/y)$$ , where $G,g$ are $C^1$ functions."




In my opinion this is not right and we are losing solutions that way.



REMARK: The only way I know we can do a similar thing is when the following PDE



$az_x+bz_y=0$ (2) is given, where $a,b$ are functions of $x,y$ and they do not vanish simultaneously. Then if $u=c$ is the general solution of the ODE:



$$frac{dx}{a}=frac{dy}{b}$$, then $z=f(u)$ , where $f$ is any $C^1$ function.



This last is taken from the book Introduction to PDE with applications by Zachamanoglou and Thoe, Example 2.2 page 62.



Is my cosideration correct?










share|cite|improve this question











$endgroup$

















    1












    $begingroup$


    I have been reading some notes about Quasi Linear PDE and I stuck to the following issue:



    Consider the PDE: $xz_x+yz_y=xe^{-z}$



    then my notes read as:




    "the general solution is: $G(x/y, e^z-x)=0$ . (1)



    and so $$e^z-x=g(x/y)$$ , where $G,g$ are $C^1$ functions."




    In my opinion this is not right and we are losing solutions that way.



    REMARK: The only way I know we can do a similar thing is when the following PDE



    $az_x+bz_y=0$ (2) is given, where $a,b$ are functions of $x,y$ and they do not vanish simultaneously. Then if $u=c$ is the general solution of the ODE:



    $$frac{dx}{a}=frac{dy}{b}$$, then $z=f(u)$ , where $f$ is any $C^1$ function.



    This last is taken from the book Introduction to PDE with applications by Zachamanoglou and Thoe, Example 2.2 page 62.



    Is my cosideration correct?










    share|cite|improve this question











    $endgroup$















      1












      1








      1





      $begingroup$


      I have been reading some notes about Quasi Linear PDE and I stuck to the following issue:



      Consider the PDE: $xz_x+yz_y=xe^{-z}$



      then my notes read as:




      "the general solution is: $G(x/y, e^z-x)=0$ . (1)



      and so $$e^z-x=g(x/y)$$ , where $G,g$ are $C^1$ functions."




      In my opinion this is not right and we are losing solutions that way.



      REMARK: The only way I know we can do a similar thing is when the following PDE



      $az_x+bz_y=0$ (2) is given, where $a,b$ are functions of $x,y$ and they do not vanish simultaneously. Then if $u=c$ is the general solution of the ODE:



      $$frac{dx}{a}=frac{dy}{b}$$, then $z=f(u)$ , where $f$ is any $C^1$ function.



      This last is taken from the book Introduction to PDE with applications by Zachamanoglou and Thoe, Example 2.2 page 62.



      Is my cosideration correct?










      share|cite|improve this question











      $endgroup$




      I have been reading some notes about Quasi Linear PDE and I stuck to the following issue:



      Consider the PDE: $xz_x+yz_y=xe^{-z}$



      then my notes read as:




      "the general solution is: $G(x/y, e^z-x)=0$ . (1)



      and so $$e^z-x=g(x/y)$$ , where $G,g$ are $C^1$ functions."




      In my opinion this is not right and we are losing solutions that way.



      REMARK: The only way I know we can do a similar thing is when the following PDE



      $az_x+bz_y=0$ (2) is given, where $a,b$ are functions of $x,y$ and they do not vanish simultaneously. Then if $u=c$ is the general solution of the ODE:



      $$frac{dx}{a}=frac{dy}{b}$$, then $z=f(u)$ , where $f$ is any $C^1$ function.



      This last is taken from the book Introduction to PDE with applications by Zachamanoglou and Thoe, Example 2.2 page 62.



      Is my cosideration correct?







      ordinary-differential-equations pde






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Dec 15 '18 at 17:09







      dmtri

















      asked Dec 14 '18 at 17:04









      dmtridmtri

      1,4822521




      1,4822521






















          1 Answer
          1






          active

          oldest

          votes


















          2












          $begingroup$

          $$xu_x+yu_y=xe^{-u}$$
          The Charpit-Lagrange equations are :
          $$frac{dx}{x}=frac{dy}{y}=frac{du}{xe^{-u}}$$
          First equation of characteristic curves , from $frac{dx}{x}=frac{dy}{y}$ :
          $$frac{x}{y}=c_1$$
          Second equation of characteristic curves , from $frac{dx}{x}=frac{du}{xe^{-u}}$:
          $$e^u-x=c_2$$
          The general solution of the PDE, expressed on the form of implicit equation is :
          $$Phileft(frac{x}{y}:,:e^u-xright)=0$$
          where $Phi$ is an arbitrary function of two variables.



          Or, equivalently on explicit form :
          $e^u-x=Fleft(frac{x}{y}right)$
          $$u(x,y)=lnleft|x+Fleft(frac{x}{y}right)right|$$
          where $F$ is an arbitrary function.



          The function $F$ had to be determined according to some boundary condition. Since there is no such condition specified in the wording of the problem, further calculus is not possible.



          Nevertheless, the above result is consistent with the solution (which is correct) noted in the OP question.






          share|cite|improve this answer











          $endgroup$













          • $begingroup$
            Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
            $endgroup$
            – dmtri
            Dec 15 '18 at 11:57








          • 1




            $begingroup$
            Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
            $endgroup$
            – JJacquelin
            Dec 15 '18 at 14:27










          • $begingroup$
            Thanks, I liked that!!, especially the kettle and fish!
            $endgroup$
            – dmtri
            Dec 15 '18 at 15:29










          • $begingroup$
            I made also some corrections to my original post, especially in the REMARK area.
            $endgroup$
            – dmtri
            Dec 15 '18 at 17:14






          • 1




            $begingroup$
            OK I agree now. So my answer about your remark area is no longer valid. I delete it.
            $endgroup$
            – JJacquelin
            Dec 16 '18 at 7:59











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          2












          $begingroup$

          $$xu_x+yu_y=xe^{-u}$$
          The Charpit-Lagrange equations are :
          $$frac{dx}{x}=frac{dy}{y}=frac{du}{xe^{-u}}$$
          First equation of characteristic curves , from $frac{dx}{x}=frac{dy}{y}$ :
          $$frac{x}{y}=c_1$$
          Second equation of characteristic curves , from $frac{dx}{x}=frac{du}{xe^{-u}}$:
          $$e^u-x=c_2$$
          The general solution of the PDE, expressed on the form of implicit equation is :
          $$Phileft(frac{x}{y}:,:e^u-xright)=0$$
          where $Phi$ is an arbitrary function of two variables.



          Or, equivalently on explicit form :
          $e^u-x=Fleft(frac{x}{y}right)$
          $$u(x,y)=lnleft|x+Fleft(frac{x}{y}right)right|$$
          where $F$ is an arbitrary function.



          The function $F$ had to be determined according to some boundary condition. Since there is no such condition specified in the wording of the problem, further calculus is not possible.



          Nevertheless, the above result is consistent with the solution (which is correct) noted in the OP question.






          share|cite|improve this answer











          $endgroup$













          • $begingroup$
            Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
            $endgroup$
            – dmtri
            Dec 15 '18 at 11:57








          • 1




            $begingroup$
            Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
            $endgroup$
            – JJacquelin
            Dec 15 '18 at 14:27










          • $begingroup$
            Thanks, I liked that!!, especially the kettle and fish!
            $endgroup$
            – dmtri
            Dec 15 '18 at 15:29










          • $begingroup$
            I made also some corrections to my original post, especially in the REMARK area.
            $endgroup$
            – dmtri
            Dec 15 '18 at 17:14






          • 1




            $begingroup$
            OK I agree now. So my answer about your remark area is no longer valid. I delete it.
            $endgroup$
            – JJacquelin
            Dec 16 '18 at 7:59
















          2












          $begingroup$

          $$xu_x+yu_y=xe^{-u}$$
          The Charpit-Lagrange equations are :
          $$frac{dx}{x}=frac{dy}{y}=frac{du}{xe^{-u}}$$
          First equation of characteristic curves , from $frac{dx}{x}=frac{dy}{y}$ :
          $$frac{x}{y}=c_1$$
          Second equation of characteristic curves , from $frac{dx}{x}=frac{du}{xe^{-u}}$:
          $$e^u-x=c_2$$
          The general solution of the PDE, expressed on the form of implicit equation is :
          $$Phileft(frac{x}{y}:,:e^u-xright)=0$$
          where $Phi$ is an arbitrary function of two variables.



          Or, equivalently on explicit form :
          $e^u-x=Fleft(frac{x}{y}right)$
          $$u(x,y)=lnleft|x+Fleft(frac{x}{y}right)right|$$
          where $F$ is an arbitrary function.



          The function $F$ had to be determined according to some boundary condition. Since there is no such condition specified in the wording of the problem, further calculus is not possible.



          Nevertheless, the above result is consistent with the solution (which is correct) noted in the OP question.






          share|cite|improve this answer











          $endgroup$













          • $begingroup$
            Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
            $endgroup$
            – dmtri
            Dec 15 '18 at 11:57








          • 1




            $begingroup$
            Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
            $endgroup$
            – JJacquelin
            Dec 15 '18 at 14:27










          • $begingroup$
            Thanks, I liked that!!, especially the kettle and fish!
            $endgroup$
            – dmtri
            Dec 15 '18 at 15:29










          • $begingroup$
            I made also some corrections to my original post, especially in the REMARK area.
            $endgroup$
            – dmtri
            Dec 15 '18 at 17:14






          • 1




            $begingroup$
            OK I agree now. So my answer about your remark area is no longer valid. I delete it.
            $endgroup$
            – JJacquelin
            Dec 16 '18 at 7:59














          2












          2








          2





          $begingroup$

          $$xu_x+yu_y=xe^{-u}$$
          The Charpit-Lagrange equations are :
          $$frac{dx}{x}=frac{dy}{y}=frac{du}{xe^{-u}}$$
          First equation of characteristic curves , from $frac{dx}{x}=frac{dy}{y}$ :
          $$frac{x}{y}=c_1$$
          Second equation of characteristic curves , from $frac{dx}{x}=frac{du}{xe^{-u}}$:
          $$e^u-x=c_2$$
          The general solution of the PDE, expressed on the form of implicit equation is :
          $$Phileft(frac{x}{y}:,:e^u-xright)=0$$
          where $Phi$ is an arbitrary function of two variables.



          Or, equivalently on explicit form :
          $e^u-x=Fleft(frac{x}{y}right)$
          $$u(x,y)=lnleft|x+Fleft(frac{x}{y}right)right|$$
          where $F$ is an arbitrary function.



          The function $F$ had to be determined according to some boundary condition. Since there is no such condition specified in the wording of the problem, further calculus is not possible.



          Nevertheless, the above result is consistent with the solution (which is correct) noted in the OP question.






          share|cite|improve this answer











          $endgroup$



          $$xu_x+yu_y=xe^{-u}$$
          The Charpit-Lagrange equations are :
          $$frac{dx}{x}=frac{dy}{y}=frac{du}{xe^{-u}}$$
          First equation of characteristic curves , from $frac{dx}{x}=frac{dy}{y}$ :
          $$frac{x}{y}=c_1$$
          Second equation of characteristic curves , from $frac{dx}{x}=frac{du}{xe^{-u}}$:
          $$e^u-x=c_2$$
          The general solution of the PDE, expressed on the form of implicit equation is :
          $$Phileft(frac{x}{y}:,:e^u-xright)=0$$
          where $Phi$ is an arbitrary function of two variables.



          Or, equivalently on explicit form :
          $e^u-x=Fleft(frac{x}{y}right)$
          $$u(x,y)=lnleft|x+Fleft(frac{x}{y}right)right|$$
          where $F$ is an arbitrary function.



          The function $F$ had to be determined according to some boundary condition. Since there is no such condition specified in the wording of the problem, further calculus is not possible.



          Nevertheless, the above result is consistent with the solution (which is correct) noted in the OP question.







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Dec 16 '18 at 8:00

























          answered Dec 15 '18 at 10:39









          JJacquelinJJacquelin

          43.7k21853




          43.7k21853












          • $begingroup$
            Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
            $endgroup$
            – dmtri
            Dec 15 '18 at 11:57








          • 1




            $begingroup$
            Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
            $endgroup$
            – JJacquelin
            Dec 15 '18 at 14:27










          • $begingroup$
            Thanks, I liked that!!, especially the kettle and fish!
            $endgroup$
            – dmtri
            Dec 15 '18 at 15:29










          • $begingroup$
            I made also some corrections to my original post, especially in the REMARK area.
            $endgroup$
            – dmtri
            Dec 15 '18 at 17:14






          • 1




            $begingroup$
            OK I agree now. So my answer about your remark area is no longer valid. I delete it.
            $endgroup$
            – JJacquelin
            Dec 16 '18 at 7:59


















          • $begingroup$
            Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
            $endgroup$
            – dmtri
            Dec 15 '18 at 11:57








          • 1




            $begingroup$
            Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
            $endgroup$
            – JJacquelin
            Dec 15 '18 at 14:27










          • $begingroup$
            Thanks, I liked that!!, especially the kettle and fish!
            $endgroup$
            – dmtri
            Dec 15 '18 at 15:29










          • $begingroup$
            I made also some corrections to my original post, especially in the REMARK area.
            $endgroup$
            – dmtri
            Dec 15 '18 at 17:14






          • 1




            $begingroup$
            OK I agree now. So my answer about your remark area is no longer valid. I delete it.
            $endgroup$
            – JJacquelin
            Dec 16 '18 at 7:59
















          $begingroup$
          Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
          $endgroup$
          – dmtri
          Dec 15 '18 at 11:57






          $begingroup$
          Thanks for the explicit answer(+25), but what I am worried about is how do You derive from the general integral $Phi(u_1,u_2)=0$ the solution: $u_2=F(u_1)$ ....especially when $Phi_{u_2}=0$...ie you cannot solve for $u_2$. Are the general integral and general solution equivalent?
          $endgroup$
          – dmtri
          Dec 15 '18 at 11:57






          1




          1




          $begingroup$
          Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
          $endgroup$
          – JJacquelin
          Dec 15 '18 at 14:27




          $begingroup$
          Of course it is not always possible to solve $Phi(u_1,u_2)=0$ for an explicit form $u_2=F(u_1)$ in terms of standard elementary and/or special functions. So, the equivalence is purely symbolic. If it is not possible today one can imagine that a convenient brand-new special function will be standardised in the futur, then allowing to do it. In any case everybody can define convenient particular special functions (Which should be of no practical use until being standardized and become common in math literature. That is a different kettle of fish).
          $endgroup$
          – JJacquelin
          Dec 15 '18 at 14:27












          $begingroup$
          Thanks, I liked that!!, especially the kettle and fish!
          $endgroup$
          – dmtri
          Dec 15 '18 at 15:29




          $begingroup$
          Thanks, I liked that!!, especially the kettle and fish!
          $endgroup$
          – dmtri
          Dec 15 '18 at 15:29












          $begingroup$
          I made also some corrections to my original post, especially in the REMARK area.
          $endgroup$
          – dmtri
          Dec 15 '18 at 17:14




          $begingroup$
          I made also some corrections to my original post, especially in the REMARK area.
          $endgroup$
          – dmtri
          Dec 15 '18 at 17:14




          1




          1




          $begingroup$
          OK I agree now. So my answer about your remark area is no longer valid. I delete it.
          $endgroup$
          – JJacquelin
          Dec 16 '18 at 7:59




          $begingroup$
          OK I agree now. So my answer about your remark area is no longer valid. I delete it.
          $endgroup$
          – JJacquelin
          Dec 16 '18 at 7:59


















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