Separating variables in a PDE with multiple constantsHow to solve this PDE?Solving one dimensonal PDESolving the Laplace equation in terms of exponential of hyperbolic trigonometric functionsPDE with periodic boundary conditionsSolving a PDE through separation of variablesPDE using separation of variablesUsing Laplace Transforms to solve a PDETextbook Example Solving Heat Conduction PDE Using Separation of VariablesProblem with satisfying Boundary conditions for 1D heat PDESolving PDE using separation of variables (Heat diffusion)

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Separating variables in a PDE with multiple constants


How to solve this PDE?Solving one dimensonal PDESolving the Laplace equation in terms of exponential of hyperbolic trigonometric functionsPDE with periodic boundary conditionsSolving a PDE through separation of variablesPDE using separation of variablesUsing Laplace Transforms to solve a PDETextbook Example Solving Heat Conduction PDE Using Separation of VariablesProblem with satisfying Boundary conditions for 1D heat PDESolving PDE using separation of variables (Heat diffusion)













0












$begingroup$


My question is:



How do you use separation of variables on a PDE that has more than one constant in it?



All the examples I can find in my book/online only have one constant in it, like $$ fracpartial upartial t=kfracpartial^2
upartial x^2+kfracpartial^2 upartial y^2$$



Which then means only one of the resultant ODEs has $k$ in it. If there is more than one constant, what do you do? Still use separation of variables? My attempt is below the question.



The problem I am working on is:




Solve



$displaystyle fracpartial upartial t=k_1fracpartial^2
upartial x^2+k_2fracpartial^2 upartial y^2$



on a rectangle $(0 lt x lt L, 0 lt y lt H)$ subject to



$displaystyle u(0,y,t)=0, fracpartial upartial y(x,0,t)=0$



$displaystyle u(0,y,0)=alpha(x,y)$



$displaystyle u(L,y,t)=0, fracpartial upartial y(x,H,t)=0$




What I have done so far:



Let $u(x,t)=X(x)Y(y)T(t)$. Then using separation of variables we have:



(1) $displaystyle fracd Td t=-lambda(k_1+k_2)T, text IC: T(0)=alpha(x,y)$



(2) $displaystyle fracd^2Xdx^2=-mu frac(k_1+k_2)Xk_1, text BCs: X(0)=0, X(L)=0$



(3) $displaystyle fracd^2Ydy^2=-(lambda - mu) frac(k_1+k_2)Yk_2, text BCs: Y'(0)=0, Y'(H)=0$










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
    $endgroup$
    – Jens Wagemaker
    Mar 11 at 20:56















0












$begingroup$


My question is:



How do you use separation of variables on a PDE that has more than one constant in it?



All the examples I can find in my book/online only have one constant in it, like $$ fracpartial upartial t=kfracpartial^2
upartial x^2+kfracpartial^2 upartial y^2$$



Which then means only one of the resultant ODEs has $k$ in it. If there is more than one constant, what do you do? Still use separation of variables? My attempt is below the question.



The problem I am working on is:




Solve



$displaystyle fracpartial upartial t=k_1fracpartial^2
upartial x^2+k_2fracpartial^2 upartial y^2$



on a rectangle $(0 lt x lt L, 0 lt y lt H)$ subject to



$displaystyle u(0,y,t)=0, fracpartial upartial y(x,0,t)=0$



$displaystyle u(0,y,0)=alpha(x,y)$



$displaystyle u(L,y,t)=0, fracpartial upartial y(x,H,t)=0$




What I have done so far:



Let $u(x,t)=X(x)Y(y)T(t)$. Then using separation of variables we have:



(1) $displaystyle fracd Td t=-lambda(k_1+k_2)T, text IC: T(0)=alpha(x,y)$



(2) $displaystyle fracd^2Xdx^2=-mu frac(k_1+k_2)Xk_1, text BCs: X(0)=0, X(L)=0$



(3) $displaystyle fracd^2Ydy^2=-(lambda - mu) frac(k_1+k_2)Yk_2, text BCs: Y'(0)=0, Y'(H)=0$










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
    $endgroup$
    – Jens Wagemaker
    Mar 11 at 20:56













0












0








0





$begingroup$


My question is:



How do you use separation of variables on a PDE that has more than one constant in it?



All the examples I can find in my book/online only have one constant in it, like $$ fracpartial upartial t=kfracpartial^2
upartial x^2+kfracpartial^2 upartial y^2$$



Which then means only one of the resultant ODEs has $k$ in it. If there is more than one constant, what do you do? Still use separation of variables? My attempt is below the question.



The problem I am working on is:




Solve



$displaystyle fracpartial upartial t=k_1fracpartial^2
upartial x^2+k_2fracpartial^2 upartial y^2$



on a rectangle $(0 lt x lt L, 0 lt y lt H)$ subject to



$displaystyle u(0,y,t)=0, fracpartial upartial y(x,0,t)=0$



$displaystyle u(0,y,0)=alpha(x,y)$



$displaystyle u(L,y,t)=0, fracpartial upartial y(x,H,t)=0$




What I have done so far:



Let $u(x,t)=X(x)Y(y)T(t)$. Then using separation of variables we have:



(1) $displaystyle fracd Td t=-lambda(k_1+k_2)T, text IC: T(0)=alpha(x,y)$



(2) $displaystyle fracd^2Xdx^2=-mu frac(k_1+k_2)Xk_1, text BCs: X(0)=0, X(L)=0$



(3) $displaystyle fracd^2Ydy^2=-(lambda - mu) frac(k_1+k_2)Yk_2, text BCs: Y'(0)=0, Y'(H)=0$










share|cite|improve this question











$endgroup$




My question is:



How do you use separation of variables on a PDE that has more than one constant in it?



All the examples I can find in my book/online only have one constant in it, like $$ fracpartial upartial t=kfracpartial^2
upartial x^2+kfracpartial^2 upartial y^2$$



Which then means only one of the resultant ODEs has $k$ in it. If there is more than one constant, what do you do? Still use separation of variables? My attempt is below the question.



The problem I am working on is:




Solve



$displaystyle fracpartial upartial t=k_1fracpartial^2
upartial x^2+k_2fracpartial^2 upartial y^2$



on a rectangle $(0 lt x lt L, 0 lt y lt H)$ subject to



$displaystyle u(0,y,t)=0, fracpartial upartial y(x,0,t)=0$



$displaystyle u(0,y,0)=alpha(x,y)$



$displaystyle u(L,y,t)=0, fracpartial upartial y(x,H,t)=0$




What I have done so far:



Let $u(x,t)=X(x)Y(y)T(t)$. Then using separation of variables we have:



(1) $displaystyle fracd Td t=-lambda(k_1+k_2)T, text IC: T(0)=alpha(x,y)$



(2) $displaystyle fracd^2Xdx^2=-mu frac(k_1+k_2)Xk_1, text BCs: X(0)=0, X(L)=0$



(3) $displaystyle fracd^2Ydy^2=-(lambda - mu) frac(k_1+k_2)Yk_2, text BCs: Y'(0)=0, Y'(H)=0$







pde boundary-value-problem heat-equation






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Mar 12 at 6:02









Dylan

13.9k31127




13.9k31127










asked Mar 11 at 20:13









LovesPeanutButterLovesPeanutButter

836




836







  • 1




    $begingroup$
    What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
    $endgroup$
    – Jens Wagemaker
    Mar 11 at 20:56












  • 1




    $begingroup$
    What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
    $endgroup$
    – Jens Wagemaker
    Mar 11 at 20:56







1




1




$begingroup$
What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
$endgroup$
– Jens Wagemaker
Mar 11 at 20:56




$begingroup$
What if you now solve these ODE's? The first gives an exponential, the second and third gives sines and cosines. That gives you $T,X$ and $Y$. And then check if $XYT$ is a solution?
$endgroup$
– Jens Wagemaker
Mar 11 at 20:56










1 Answer
1






active

oldest

votes


















2












$begingroup$

You could also change the order of the assignment of variables. In
$$
fracT'(t)T(t)=k_1fracX''(x)X(x)+k_2fracY''(y)Y(y)
$$

all terms must be constants, so that you can set $fracX''(x)X(x)=-λ$, $fracY''(y)Y(y)=-μ$ and thus in consequence $fracT'(t)T(t)=-(k_1λ+k_2μ)$. I think the expressions for the constants in this form are less complex.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
    $endgroup$
    – LovesPeanutButter
    Mar 11 at 21:48







  • 1




    $begingroup$
    Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
    $endgroup$
    – LutzL
    Mar 11 at 23:22










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1 Answer
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oldest

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1 Answer
1






active

oldest

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active

oldest

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active

oldest

votes









2












$begingroup$

You could also change the order of the assignment of variables. In
$$
fracT'(t)T(t)=k_1fracX''(x)X(x)+k_2fracY''(y)Y(y)
$$

all terms must be constants, so that you can set $fracX''(x)X(x)=-λ$, $fracY''(y)Y(y)=-μ$ and thus in consequence $fracT'(t)T(t)=-(k_1λ+k_2μ)$. I think the expressions for the constants in this form are less complex.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
    $endgroup$
    – LovesPeanutButter
    Mar 11 at 21:48







  • 1




    $begingroup$
    Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
    $endgroup$
    – LutzL
    Mar 11 at 23:22















2












$begingroup$

You could also change the order of the assignment of variables. In
$$
fracT'(t)T(t)=k_1fracX''(x)X(x)+k_2fracY''(y)Y(y)
$$

all terms must be constants, so that you can set $fracX''(x)X(x)=-λ$, $fracY''(y)Y(y)=-μ$ and thus in consequence $fracT'(t)T(t)=-(k_1λ+k_2μ)$. I think the expressions for the constants in this form are less complex.






share|cite|improve this answer









$endgroup$












  • $begingroup$
    So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
    $endgroup$
    – LovesPeanutButter
    Mar 11 at 21:48







  • 1




    $begingroup$
    Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
    $endgroup$
    – LutzL
    Mar 11 at 23:22













2












2








2





$begingroup$

You could also change the order of the assignment of variables. In
$$
fracT'(t)T(t)=k_1fracX''(x)X(x)+k_2fracY''(y)Y(y)
$$

all terms must be constants, so that you can set $fracX''(x)X(x)=-λ$, $fracY''(y)Y(y)=-μ$ and thus in consequence $fracT'(t)T(t)=-(k_1λ+k_2μ)$. I think the expressions for the constants in this form are less complex.






share|cite|improve this answer









$endgroup$



You could also change the order of the assignment of variables. In
$$
fracT'(t)T(t)=k_1fracX''(x)X(x)+k_2fracY''(y)Y(y)
$$

all terms must be constants, so that you can set $fracX''(x)X(x)=-λ$, $fracY''(y)Y(y)=-μ$ and thus in consequence $fracT'(t)T(t)=-(k_1λ+k_2μ)$. I think the expressions for the constants in this form are less complex.







share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Mar 11 at 21:08









LutzLLutzL

59.6k42057




59.6k42057











  • $begingroup$
    So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
    $endgroup$
    – LovesPeanutButter
    Mar 11 at 21:48







  • 1




    $begingroup$
    Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
    $endgroup$
    – LutzL
    Mar 11 at 23:22
















  • $begingroup$
    So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
    $endgroup$
    – LovesPeanutButter
    Mar 11 at 21:48







  • 1




    $begingroup$
    Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
    $endgroup$
    – LutzL
    Mar 11 at 23:22















$begingroup$
So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
$endgroup$
– LovesPeanutButter
Mar 11 at 21:48





$begingroup$
So using this method, the three ODEs to solve become: (1) $displaystyle X''+lambda X=0, text BCs: X(0)=0, X(L)=0$ (2) $displaystyle Y''+mu Y=0, text BCs: Y'(0)=0, Y'(H)=0$ (3) $displaystyle T'+(k_1 lambda +k_2 mu)T=0, text IC: T(0)=alpha(x,y)$ ?
$endgroup$
– LovesPeanutButter
Mar 11 at 21:48





1




1




$begingroup$
Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
$endgroup$
– LutzL
Mar 11 at 23:22




$begingroup$
Yes up to the last condition. The IC for $T$ is the Fourier coefficient corresponding to $(λ,μ)$ in the expansion of the initial function $α$ in the eigenbasis.
$endgroup$
– LutzL
Mar 11 at 23:22

















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