Solution to this second order linear differential equation with variable coefficients The Next CEO of Stack OverflowA second-order non-linear differential equationSecond order linear differential equationSecond order homogeneous differential equation with non-constant coefficientsParticular second order differential equation with variable coefficientssecond order linear differential equation with variable coefficientsSecond order linear homogeneous differential equation with variable coefficientsSolving a 2-variable Second Order Linear Partial Differential EquationSecond order linear partial differential equation with complex coefficients.Solving Second Order differential equation using Variation of ParametersSecond order homogenous differential equation with variable coefficients

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Solution to this second order linear differential equation with variable coefficients



The Next CEO of Stack OverflowA second-order non-linear differential equationSecond order linear differential equationSecond order homogeneous differential equation with non-constant coefficientsParticular second order differential equation with variable coefficientssecond order linear differential equation with variable coefficientsSecond order linear homogeneous differential equation with variable coefficientsSolving a 2-variable Second Order Linear Partial Differential EquationSecond order linear partial differential equation with complex coefficients.Solving Second Order differential equation using Variation of ParametersSecond order homogenous differential equation with variable coefficients










2












$begingroup$


I have the following second order linear ordinary differential equation with variable coefficients:



$ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = varphi(E,0)$, where $overlinevarphi = overlinevarphi(E,s) = int_0^infty varphi(E,x)e^-sxdx$.



Before I actually show how I tried to solve this, it is perhaps good if I provide some background. This equation is obtained by taking the Laplace transform in the x variable of the following second order partial differential equation:



$c cdot fracpartial^2 varphi(E,x)partial E^2 + aE^k cdot fracpartial varphi(E,x)partial E + akE^k-1 cdot varphi + fracpartial varphipartial x = 0 $ where $E in (infty,+infty) , xin(0,infty)$ .



Coming back to the first equation, in order to solve this I have attempted to reduce this to an equation with constant coefficients, by following this document: http://www.mecheng.iisc.ernet.in/~sonti/ME261_variable_coeff_2nd_order.pdf.



However, when calculating whether the equation is exact, via the $P''-Q'+R$ formula, the result is the $s $ constant. Thus, I have concluded that the equation cannot be reduced to an equation with constant coefficients.



I have also tried using the variation of parameters on the equation. This was mostly by following the method given here: http://tutorial.math.lamar.edu/Classes/DE/VariationofParameters.aspx



However, that requires knowledge of the fundamental solutions of the equation. The fundamental solutions are obtained by solving the following equation:



$ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = 0$



I attempted thereafter to solve the following polynomial:



$cr^2+aE^kr+(akE^k-1+s)=0$



The constants in the equation are: $c = 0.1/2$, $a = e^148$ and $k = -1.4$. When I plotted the delta from the well known abc formula it always turned out positive. So I have concluded that the roots of the equation are real and thus the fundamental solutions are



$overlinevarphi_1 = e^Er_1(s)$ and $overlinevarphi_2 = e^Er_2(s)$, with $r_1$ and $r_2$ the roots of the characteristic polynomial.



Thus, the variation of parameters method states that the solution to this equation is:



$overlinevarphi(E,s) = -overlinevarphi_1 int_0^infty fracoverlinevarphi_2varphi(E,0)W(overlinevarphi_1,overlinevarphi_2) + overlinevarphi_2 int_0^infty fracoverlinevarphi_1varphi(E,0)W(overlinevarphi_1,overlinevarphi_2)$



Using this the solution to the original PDE can be obtained via:



$varphi(E,x) = frac12pi iint_gamma-iinfty^gamma+iinfty overlinevarphi(E,s)e^sxds$



So, my questions are:



  1. Does the first equation in the post have an analytical solution?

  2. Is my treatment correct?

  3. Do you have suggestions for improvements/ alternative methods?

Thank you in advance










share|cite|improve this question







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Tiberiu is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
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    2












    $begingroup$


    I have the following second order linear ordinary differential equation with variable coefficients:



    $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = varphi(E,0)$, where $overlinevarphi = overlinevarphi(E,s) = int_0^infty varphi(E,x)e^-sxdx$.



    Before I actually show how I tried to solve this, it is perhaps good if I provide some background. This equation is obtained by taking the Laplace transform in the x variable of the following second order partial differential equation:



    $c cdot fracpartial^2 varphi(E,x)partial E^2 + aE^k cdot fracpartial varphi(E,x)partial E + akE^k-1 cdot varphi + fracpartial varphipartial x = 0 $ where $E in (infty,+infty) , xin(0,infty)$ .



    Coming back to the first equation, in order to solve this I have attempted to reduce this to an equation with constant coefficients, by following this document: http://www.mecheng.iisc.ernet.in/~sonti/ME261_variable_coeff_2nd_order.pdf.



    However, when calculating whether the equation is exact, via the $P''-Q'+R$ formula, the result is the $s $ constant. Thus, I have concluded that the equation cannot be reduced to an equation with constant coefficients.



    I have also tried using the variation of parameters on the equation. This was mostly by following the method given here: http://tutorial.math.lamar.edu/Classes/DE/VariationofParameters.aspx



    However, that requires knowledge of the fundamental solutions of the equation. The fundamental solutions are obtained by solving the following equation:



    $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = 0$



    I attempted thereafter to solve the following polynomial:



    $cr^2+aE^kr+(akE^k-1+s)=0$



    The constants in the equation are: $c = 0.1/2$, $a = e^148$ and $k = -1.4$. When I plotted the delta from the well known abc formula it always turned out positive. So I have concluded that the roots of the equation are real and thus the fundamental solutions are



    $overlinevarphi_1 = e^Er_1(s)$ and $overlinevarphi_2 = e^Er_2(s)$, with $r_1$ and $r_2$ the roots of the characteristic polynomial.



    Thus, the variation of parameters method states that the solution to this equation is:



    $overlinevarphi(E,s) = -overlinevarphi_1 int_0^infty fracoverlinevarphi_2varphi(E,0)W(overlinevarphi_1,overlinevarphi_2) + overlinevarphi_2 int_0^infty fracoverlinevarphi_1varphi(E,0)W(overlinevarphi_1,overlinevarphi_2)$



    Using this the solution to the original PDE can be obtained via:



    $varphi(E,x) = frac12pi iint_gamma-iinfty^gamma+iinfty overlinevarphi(E,s)e^sxds$



    So, my questions are:



    1. Does the first equation in the post have an analytical solution?

    2. Is my treatment correct?

    3. Do you have suggestions for improvements/ alternative methods?

    Thank you in advance










    share|cite|improve this question







    New contributor




    Tiberiu is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.







    $endgroup$














      2












      2








      2


      1



      $begingroup$


      I have the following second order linear ordinary differential equation with variable coefficients:



      $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = varphi(E,0)$, where $overlinevarphi = overlinevarphi(E,s) = int_0^infty varphi(E,x)e^-sxdx$.



      Before I actually show how I tried to solve this, it is perhaps good if I provide some background. This equation is obtained by taking the Laplace transform in the x variable of the following second order partial differential equation:



      $c cdot fracpartial^2 varphi(E,x)partial E^2 + aE^k cdot fracpartial varphi(E,x)partial E + akE^k-1 cdot varphi + fracpartial varphipartial x = 0 $ where $E in (infty,+infty) , xin(0,infty)$ .



      Coming back to the first equation, in order to solve this I have attempted to reduce this to an equation with constant coefficients, by following this document: http://www.mecheng.iisc.ernet.in/~sonti/ME261_variable_coeff_2nd_order.pdf.



      However, when calculating whether the equation is exact, via the $P''-Q'+R$ formula, the result is the $s $ constant. Thus, I have concluded that the equation cannot be reduced to an equation with constant coefficients.



      I have also tried using the variation of parameters on the equation. This was mostly by following the method given here: http://tutorial.math.lamar.edu/Classes/DE/VariationofParameters.aspx



      However, that requires knowledge of the fundamental solutions of the equation. The fundamental solutions are obtained by solving the following equation:



      $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = 0$



      I attempted thereafter to solve the following polynomial:



      $cr^2+aE^kr+(akE^k-1+s)=0$



      The constants in the equation are: $c = 0.1/2$, $a = e^148$ and $k = -1.4$. When I plotted the delta from the well known abc formula it always turned out positive. So I have concluded that the roots of the equation are real and thus the fundamental solutions are



      $overlinevarphi_1 = e^Er_1(s)$ and $overlinevarphi_2 = e^Er_2(s)$, with $r_1$ and $r_2$ the roots of the characteristic polynomial.



      Thus, the variation of parameters method states that the solution to this equation is:



      $overlinevarphi(E,s) = -overlinevarphi_1 int_0^infty fracoverlinevarphi_2varphi(E,0)W(overlinevarphi_1,overlinevarphi_2) + overlinevarphi_2 int_0^infty fracoverlinevarphi_1varphi(E,0)W(overlinevarphi_1,overlinevarphi_2)$



      Using this the solution to the original PDE can be obtained via:



      $varphi(E,x) = frac12pi iint_gamma-iinfty^gamma+iinfty overlinevarphi(E,s)e^sxds$



      So, my questions are:



      1. Does the first equation in the post have an analytical solution?

      2. Is my treatment correct?

      3. Do you have suggestions for improvements/ alternative methods?

      Thank you in advance










      share|cite|improve this question







      New contributor




      Tiberiu is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
      Check out our Code of Conduct.







      $endgroup$




      I have the following second order linear ordinary differential equation with variable coefficients:



      $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = varphi(E,0)$, where $overlinevarphi = overlinevarphi(E,s) = int_0^infty varphi(E,x)e^-sxdx$.



      Before I actually show how I tried to solve this, it is perhaps good if I provide some background. This equation is obtained by taking the Laplace transform in the x variable of the following second order partial differential equation:



      $c cdot fracpartial^2 varphi(E,x)partial E^2 + aE^k cdot fracpartial varphi(E,x)partial E + akE^k-1 cdot varphi + fracpartial varphipartial x = 0 $ where $E in (infty,+infty) , xin(0,infty)$ .



      Coming back to the first equation, in order to solve this I have attempted to reduce this to an equation with constant coefficients, by following this document: http://www.mecheng.iisc.ernet.in/~sonti/ME261_variable_coeff_2nd_order.pdf.



      However, when calculating whether the equation is exact, via the $P''-Q'+R$ formula, the result is the $s $ constant. Thus, I have concluded that the equation cannot be reduced to an equation with constant coefficients.



      I have also tried using the variation of parameters on the equation. This was mostly by following the method given here: http://tutorial.math.lamar.edu/Classes/DE/VariationofParameters.aspx



      However, that requires knowledge of the fundamental solutions of the equation. The fundamental solutions are obtained by solving the following equation:



      $ c fracd^2 overlinevarphid E^2 + aE^k fracd overlinevarphid E + (akE^k-1 +s)overlinevarphi = 0$



      I attempted thereafter to solve the following polynomial:



      $cr^2+aE^kr+(akE^k-1+s)=0$



      The constants in the equation are: $c = 0.1/2$, $a = e^148$ and $k = -1.4$. When I plotted the delta from the well known abc formula it always turned out positive. So I have concluded that the roots of the equation are real and thus the fundamental solutions are



      $overlinevarphi_1 = e^Er_1(s)$ and $overlinevarphi_2 = e^Er_2(s)$, with $r_1$ and $r_2$ the roots of the characteristic polynomial.



      Thus, the variation of parameters method states that the solution to this equation is:



      $overlinevarphi(E,s) = -overlinevarphi_1 int_0^infty fracoverlinevarphi_2varphi(E,0)W(overlinevarphi_1,overlinevarphi_2) + overlinevarphi_2 int_0^infty fracoverlinevarphi_1varphi(E,0)W(overlinevarphi_1,overlinevarphi_2)$



      Using this the solution to the original PDE can be obtained via:



      $varphi(E,x) = frac12pi iint_gamma-iinfty^gamma+iinfty overlinevarphi(E,s)e^sxds$



      So, my questions are:



      1. Does the first equation in the post have an analytical solution?

      2. Is my treatment correct?

      3. Do you have suggestions for improvements/ alternative methods?

      Thank you in advance







      ordinary-differential-equations pde laplace-transform






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      Tiberiu is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
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      asked Mar 28 at 10:50









      TiberiuTiberiu

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          1 Answer
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          $begingroup$

          Hint:



          For $cdfracd^2overlinevarphidE^2+aE^kdfracdoverlinevarphidE+(akE^k-1+s)overlinevarphi=0$ ,



          Let $overlinevarphi=e^mEoverline U$ ,



          Then $dfracdoverlinevarphidE=e^mEdfracdoverline UdE+me^mEoverline U$



          $dfracd^2overlinevarphidE^2=e^mEdfracd^2overline UdE^2+me^mEdfracdoverline UdE+me^mEdfracdoverline UdE+m^2e^mEoverline U=e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline U$



          $therefore cleft(e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline Uright)+aE^kleft(e^mEdfracdoverline UdE+me^mEoverline Uright)+(akE^k-1+s)e^mEoverline U=0$



          $cleft(dfracd^2overline UdE^2+2mdfracdoverline UdE+m^2overline Uright)+aE^kleft(dfracdoverline UdE+moverline Uright)+(akE^k-1+s)overline U=0$



          $cdfracd^2overline UdE^2+(aE^k+2cm)dfracdoverline UdE+(amE^k+akE^k-1+cm^2+s)overline U=0$



          Take $cm^2+s=0$ , i.e. $m=pm isqrtdfracsc$ , the ODE becomes



          $cdfracd^2overline UdE^2+(aE^kpm2isqrtcs)dfracdoverline UdE+left(pm iasqrtdfracscE^k+akE^k-1right)overline U=0$






          share|cite|improve this answer









          $endgroup$













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            1 Answer
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            1 Answer
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            0












            $begingroup$

            Hint:



            For $cdfracd^2overlinevarphidE^2+aE^kdfracdoverlinevarphidE+(akE^k-1+s)overlinevarphi=0$ ,



            Let $overlinevarphi=e^mEoverline U$ ,



            Then $dfracdoverlinevarphidE=e^mEdfracdoverline UdE+me^mEoverline U$



            $dfracd^2overlinevarphidE^2=e^mEdfracd^2overline UdE^2+me^mEdfracdoverline UdE+me^mEdfracdoverline UdE+m^2e^mEoverline U=e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline U$



            $therefore cleft(e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline Uright)+aE^kleft(e^mEdfracdoverline UdE+me^mEoverline Uright)+(akE^k-1+s)e^mEoverline U=0$



            $cleft(dfracd^2overline UdE^2+2mdfracdoverline UdE+m^2overline Uright)+aE^kleft(dfracdoverline UdE+moverline Uright)+(akE^k-1+s)overline U=0$



            $cdfracd^2overline UdE^2+(aE^k+2cm)dfracdoverline UdE+(amE^k+akE^k-1+cm^2+s)overline U=0$



            Take $cm^2+s=0$ , i.e. $m=pm isqrtdfracsc$ , the ODE becomes



            $cdfracd^2overline UdE^2+(aE^kpm2isqrtcs)dfracdoverline UdE+left(pm iasqrtdfracscE^k+akE^k-1right)overline U=0$






            share|cite|improve this answer









            $endgroup$

















              0












              $begingroup$

              Hint:



              For $cdfracd^2overlinevarphidE^2+aE^kdfracdoverlinevarphidE+(akE^k-1+s)overlinevarphi=0$ ,



              Let $overlinevarphi=e^mEoverline U$ ,



              Then $dfracdoverlinevarphidE=e^mEdfracdoverline UdE+me^mEoverline U$



              $dfracd^2overlinevarphidE^2=e^mEdfracd^2overline UdE^2+me^mEdfracdoverline UdE+me^mEdfracdoverline UdE+m^2e^mEoverline U=e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline U$



              $therefore cleft(e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline Uright)+aE^kleft(e^mEdfracdoverline UdE+me^mEoverline Uright)+(akE^k-1+s)e^mEoverline U=0$



              $cleft(dfracd^2overline UdE^2+2mdfracdoverline UdE+m^2overline Uright)+aE^kleft(dfracdoverline UdE+moverline Uright)+(akE^k-1+s)overline U=0$



              $cdfracd^2overline UdE^2+(aE^k+2cm)dfracdoverline UdE+(amE^k+akE^k-1+cm^2+s)overline U=0$



              Take $cm^2+s=0$ , i.e. $m=pm isqrtdfracsc$ , the ODE becomes



              $cdfracd^2overline UdE^2+(aE^kpm2isqrtcs)dfracdoverline UdE+left(pm iasqrtdfracscE^k+akE^k-1right)overline U=0$






              share|cite|improve this answer









              $endgroup$















                0












                0








                0





                $begingroup$

                Hint:



                For $cdfracd^2overlinevarphidE^2+aE^kdfracdoverlinevarphidE+(akE^k-1+s)overlinevarphi=0$ ,



                Let $overlinevarphi=e^mEoverline U$ ,



                Then $dfracdoverlinevarphidE=e^mEdfracdoverline UdE+me^mEoverline U$



                $dfracd^2overlinevarphidE^2=e^mEdfracd^2overline UdE^2+me^mEdfracdoverline UdE+me^mEdfracdoverline UdE+m^2e^mEoverline U=e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline U$



                $therefore cleft(e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline Uright)+aE^kleft(e^mEdfracdoverline UdE+me^mEoverline Uright)+(akE^k-1+s)e^mEoverline U=0$



                $cleft(dfracd^2overline UdE^2+2mdfracdoverline UdE+m^2overline Uright)+aE^kleft(dfracdoverline UdE+moverline Uright)+(akE^k-1+s)overline U=0$



                $cdfracd^2overline UdE^2+(aE^k+2cm)dfracdoverline UdE+(amE^k+akE^k-1+cm^2+s)overline U=0$



                Take $cm^2+s=0$ , i.e. $m=pm isqrtdfracsc$ , the ODE becomes



                $cdfracd^2overline UdE^2+(aE^kpm2isqrtcs)dfracdoverline UdE+left(pm iasqrtdfracscE^k+akE^k-1right)overline U=0$






                share|cite|improve this answer









                $endgroup$



                Hint:



                For $cdfracd^2overlinevarphidE^2+aE^kdfracdoverlinevarphidE+(akE^k-1+s)overlinevarphi=0$ ,



                Let $overlinevarphi=e^mEoverline U$ ,



                Then $dfracdoverlinevarphidE=e^mEdfracdoverline UdE+me^mEoverline U$



                $dfracd^2overlinevarphidE^2=e^mEdfracd^2overline UdE^2+me^mEdfracdoverline UdE+me^mEdfracdoverline UdE+m^2e^mEoverline U=e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline U$



                $therefore cleft(e^mEdfracd^2overline UdE^2+2me^mEdfracdoverline UdE+m^2e^mEoverline Uright)+aE^kleft(e^mEdfracdoverline UdE+me^mEoverline Uright)+(akE^k-1+s)e^mEoverline U=0$



                $cleft(dfracd^2overline UdE^2+2mdfracdoverline UdE+m^2overline Uright)+aE^kleft(dfracdoverline UdE+moverline Uright)+(akE^k-1+s)overline U=0$



                $cdfracd^2overline UdE^2+(aE^k+2cm)dfracdoverline UdE+(amE^k+akE^k-1+cm^2+s)overline U=0$



                Take $cm^2+s=0$ , i.e. $m=pm isqrtdfracsc$ , the ODE becomes



                $cdfracd^2overline UdE^2+(aE^kpm2isqrtcs)dfracdoverline UdE+left(pm iasqrtdfracscE^k+akE^k-1right)overline U=0$







                share|cite|improve this answer












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                share|cite|improve this answer










                answered Mar 29 at 6:23









                doraemonpauldoraemonpaul

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