Laplace's Equation in the semi infinite strip












0












$begingroup$


The problem is $$Delta u = 0$$ in the semi infinite strip $S = {(x,y)|0<x<1,y>0}$ subject to the boundary conditions $$
begin{cases}
u(0,y) = 0, yge0\
u(1,y) = 0, yge0\
u(x,0) = f(x), 0le x le 1
end{cases}
$$

where $f$ is a given function with $f(0) = f(1) = 0$. Write $$f(x) = sum_{n=1}^{infty} a_nsin(npi x)$$ and expand the general solution in terms of the special solutions given by $u_n(x,y) = e^{-n pi y}sin(n pi x)$.



The above is the problem.



So by using separation of variables and analyzing the first two boundary conditions, I got $u(x,y) = sum_{n=1}^{infty} sin(npi x)(C_n e^{-n pi y}+D_n e^{n pi y})$, where $C_n$ and $D_n$ are constants. My question is if I could get rid of the $e^{n pi y}$ part from the general solution. I've seen someone did so but usually the boundary conditions would include for example $lim_{ytoinfty} u(x,y)$ is finite. But here the boundary conditions do not say something like this. Can I still get rid of that part based on the give information? I'm a bit confused since the later instructions of the problem seem to suggest only $e^{-n pi y}$ part remains.



Thank you so much for any insights.










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  • 1




    $begingroup$
    Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
    $endgroup$
    – Dylan
    Feb 3 at 9:00


















0












$begingroup$


The problem is $$Delta u = 0$$ in the semi infinite strip $S = {(x,y)|0<x<1,y>0}$ subject to the boundary conditions $$
begin{cases}
u(0,y) = 0, yge0\
u(1,y) = 0, yge0\
u(x,0) = f(x), 0le x le 1
end{cases}
$$

where $f$ is a given function with $f(0) = f(1) = 0$. Write $$f(x) = sum_{n=1}^{infty} a_nsin(npi x)$$ and expand the general solution in terms of the special solutions given by $u_n(x,y) = e^{-n pi y}sin(n pi x)$.



The above is the problem.



So by using separation of variables and analyzing the first two boundary conditions, I got $u(x,y) = sum_{n=1}^{infty} sin(npi x)(C_n e^{-n pi y}+D_n e^{n pi y})$, where $C_n$ and $D_n$ are constants. My question is if I could get rid of the $e^{n pi y}$ part from the general solution. I've seen someone did so but usually the boundary conditions would include for example $lim_{ytoinfty} u(x,y)$ is finite. But here the boundary conditions do not say something like this. Can I still get rid of that part based on the give information? I'm a bit confused since the later instructions of the problem seem to suggest only $e^{-n pi y}$ part remains.



Thank you so much for any insights.










share|cite|improve this question









$endgroup$








  • 1




    $begingroup$
    Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
    $endgroup$
    – Dylan
    Feb 3 at 9:00
















0












0








0





$begingroup$


The problem is $$Delta u = 0$$ in the semi infinite strip $S = {(x,y)|0<x<1,y>0}$ subject to the boundary conditions $$
begin{cases}
u(0,y) = 0, yge0\
u(1,y) = 0, yge0\
u(x,0) = f(x), 0le x le 1
end{cases}
$$

where $f$ is a given function with $f(0) = f(1) = 0$. Write $$f(x) = sum_{n=1}^{infty} a_nsin(npi x)$$ and expand the general solution in terms of the special solutions given by $u_n(x,y) = e^{-n pi y}sin(n pi x)$.



The above is the problem.



So by using separation of variables and analyzing the first two boundary conditions, I got $u(x,y) = sum_{n=1}^{infty} sin(npi x)(C_n e^{-n pi y}+D_n e^{n pi y})$, where $C_n$ and $D_n$ are constants. My question is if I could get rid of the $e^{n pi y}$ part from the general solution. I've seen someone did so but usually the boundary conditions would include for example $lim_{ytoinfty} u(x,y)$ is finite. But here the boundary conditions do not say something like this. Can I still get rid of that part based on the give information? I'm a bit confused since the later instructions of the problem seem to suggest only $e^{-n pi y}$ part remains.



Thank you so much for any insights.










share|cite|improve this question









$endgroup$




The problem is $$Delta u = 0$$ in the semi infinite strip $S = {(x,y)|0<x<1,y>0}$ subject to the boundary conditions $$
begin{cases}
u(0,y) = 0, yge0\
u(1,y) = 0, yge0\
u(x,0) = f(x), 0le x le 1
end{cases}
$$

where $f$ is a given function with $f(0) = f(1) = 0$. Write $$f(x) = sum_{n=1}^{infty} a_nsin(npi x)$$ and expand the general solution in terms of the special solutions given by $u_n(x,y) = e^{-n pi y}sin(n pi x)$.



The above is the problem.



So by using separation of variables and analyzing the first two boundary conditions, I got $u(x,y) = sum_{n=1}^{infty} sin(npi x)(C_n e^{-n pi y}+D_n e^{n pi y})$, where $C_n$ and $D_n$ are constants. My question is if I could get rid of the $e^{n pi y}$ part from the general solution. I've seen someone did so but usually the boundary conditions would include for example $lim_{ytoinfty} u(x,y)$ is finite. But here the boundary conditions do not say something like this. Can I still get rid of that part based on the give information? I'm a bit confused since the later instructions of the problem seem to suggest only $e^{-n pi y}$ part remains.



Thank you so much for any insights.







pde boundary-value-problem






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asked Feb 3 at 6:09









xf16xf16

937




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  • 1




    $begingroup$
    Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
    $endgroup$
    – Dylan
    Feb 3 at 9:00
















  • 1




    $begingroup$
    Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
    $endgroup$
    – Dylan
    Feb 3 at 9:00










1




1




$begingroup$
Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
$endgroup$
– Dylan
Feb 3 at 9:00






$begingroup$
Unfortunately you need two conditions to determine two constants. The solution may be implied to be bounded at $y to infty$ which would give $D_n=0$
$endgroup$
– Dylan
Feb 3 at 9:00












1 Answer
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Yes, there is one condition missing, as your semi-infinite strip has, very simply put, four boundary segments, at $x in {0,1}$ and at $y in {0,infty}$. But you have prescribed conditions on only three of the boundary segments so far, which leaves you with arbitrary constants in the solution (you obtain $C_n + D_n = a_n$ where only $a_n$ is known).



The boundedness of the solution as $y rightarrow infty$ usually follows from some physical considerations.






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    $begingroup$

    Yes, there is one condition missing, as your semi-infinite strip has, very simply put, four boundary segments, at $x in {0,1}$ and at $y in {0,infty}$. But you have prescribed conditions on only three of the boundary segments so far, which leaves you with arbitrary constants in the solution (you obtain $C_n + D_n = a_n$ where only $a_n$ is known).



    The boundedness of the solution as $y rightarrow infty$ usually follows from some physical considerations.






    share|cite|improve this answer











    $endgroup$


















      0












      $begingroup$

      Yes, there is one condition missing, as your semi-infinite strip has, very simply put, four boundary segments, at $x in {0,1}$ and at $y in {0,infty}$. But you have prescribed conditions on only three of the boundary segments so far, which leaves you with arbitrary constants in the solution (you obtain $C_n + D_n = a_n$ where only $a_n$ is known).



      The boundedness of the solution as $y rightarrow infty$ usually follows from some physical considerations.






      share|cite|improve this answer











      $endgroup$
















        0












        0








        0





        $begingroup$

        Yes, there is one condition missing, as your semi-infinite strip has, very simply put, four boundary segments, at $x in {0,1}$ and at $y in {0,infty}$. But you have prescribed conditions on only three of the boundary segments so far, which leaves you with arbitrary constants in the solution (you obtain $C_n + D_n = a_n$ where only $a_n$ is known).



        The boundedness of the solution as $y rightarrow infty$ usually follows from some physical considerations.






        share|cite|improve this answer











        $endgroup$



        Yes, there is one condition missing, as your semi-infinite strip has, very simply put, four boundary segments, at $x in {0,1}$ and at $y in {0,infty}$. But you have prescribed conditions on only three of the boundary segments so far, which leaves you with arbitrary constants in the solution (you obtain $C_n + D_n = a_n$ where only $a_n$ is known).



        The boundedness of the solution as $y rightarrow infty$ usually follows from some physical considerations.







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Feb 3 at 7:54

























        answered Feb 3 at 7:36









        ChristophChristoph

        59616




        59616






























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