A problem about fundamental solution of Laplace equation











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I would like to derive a solution to the following equation in $R^{3}$:



$$-Delta u(x) + e^{u(x)} - e^{-u(x)} = delta(x)$$where $Delta$ is the Laplace Operator and $delta(x)$ is the Dirac's delta function.



I know how to solve $-Delta u(x) = delta(x)$ in the sense of weak convergence but I'm stuck on the exponential term of the equation above.










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  • 3




    This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
    – Fabian
    Nov 18 at 12:22










  • One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
    – Daniele Tampieri
    Nov 18 at 13:02












  • I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
    – YC_Xu
    Nov 18 at 14:12

















up vote
2
down vote

favorite
2












I would like to derive a solution to the following equation in $R^{3}$:



$$-Delta u(x) + e^{u(x)} - e^{-u(x)} = delta(x)$$where $Delta$ is the Laplace Operator and $delta(x)$ is the Dirac's delta function.



I know how to solve $-Delta u(x) = delta(x)$ in the sense of weak convergence but I'm stuck on the exponential term of the equation above.










share|cite|improve this question




















  • 3




    This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
    – Fabian
    Nov 18 at 12:22










  • One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
    – Daniele Tampieri
    Nov 18 at 13:02












  • I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
    – YC_Xu
    Nov 18 at 14:12















up vote
2
down vote

favorite
2









up vote
2
down vote

favorite
2






2





I would like to derive a solution to the following equation in $R^{3}$:



$$-Delta u(x) + e^{u(x)} - e^{-u(x)} = delta(x)$$where $Delta$ is the Laplace Operator and $delta(x)$ is the Dirac's delta function.



I know how to solve $-Delta u(x) = delta(x)$ in the sense of weak convergence but I'm stuck on the exponential term of the equation above.










share|cite|improve this question















I would like to derive a solution to the following equation in $R^{3}$:



$$-Delta u(x) + e^{u(x)} - e^{-u(x)} = delta(x)$$where $Delta$ is the Laplace Operator and $delta(x)$ is the Dirac's delta function.



I know how to solve $-Delta u(x) = delta(x)$ in the sense of weak convergence but I'm stuck on the exponential term of the equation above.







pde heat-equation fundamental-solution






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edited Nov 18 at 13:47

























asked Nov 18 at 12:14









YC_Xu

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  • 3




    This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
    – Fabian
    Nov 18 at 12:22










  • One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
    – Daniele Tampieri
    Nov 18 at 13:02












  • I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
    – YC_Xu
    Nov 18 at 14:12
















  • 3




    This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
    – Fabian
    Nov 18 at 12:22










  • One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
    – Daniele Tampieri
    Nov 18 at 13:02












  • I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
    – YC_Xu
    Nov 18 at 14:12










3




3




This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
– Fabian
Nov 18 at 12:22




This problem is highly nonlinear. The problem is thus much harder than the simple Laplace equation which you compare it to. Could you explain a bit more about the context? (Otherwise, you might not obtain any answer to this rather hard problem)
– Fabian
Nov 18 at 12:22












One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
– Daniele Tampieri
Nov 18 at 13:02






One of the consequences of the nonlinearity of the problem, pointed out by @Fabian, is that its solvability, when the initial/boundary/source data is a measure is not guaranteed. See for example H. Brezis and A. Friedman; Nonlinear parabolic equations involving measures as initial conditions, J. Math. Pures Appl. 62 (1983), p. 73-97 for parabolic equations.
– Daniele Tampieri
Nov 18 at 13:02














I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
– YC_Xu
Nov 18 at 14:12






I guess it is reasonable to derive a solution that is radially symmetric, which reduces the equation to a nonlinear ODE. My attempt is to first solve the homogeneous ODE with right hand side being zero, i.e $-frac{d^{2}u}{dr^{2}}-frac{2}{r}u(r)+e^{u(r)}-e^{-u(r)}=0$. Then hopefully I can pick some terms in the general solution which has a singularity at zero leading to a candidate solution. However, I don't know how to solve the ODE.
– YC_Xu
Nov 18 at 14:12

















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