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How to solve these kind nonhomogeneous heat equation [on hold]


Heat-Equation with different initial valuesNonhomogeneous heat equationHow to solve this nonhomogeneous heat equationHow to solve this instance of the heat equation?Solve the initial value problem, heat equation. What method to use.Fundamental solution for 1D nonhomogeneous wave equationHow to solve heat equationHow solve next heat equation?Solving the Heat Equation using the Fourier TransformSolving heat equation variant













0












$begingroup$



Solve
$$begincases
u_t-u_xx=frac12xt &textfor 0lt xlt pi, tgt0\
u(0,t)=u(pi,t)=0 \
u(x,0) = sin x \
endcases$$




How to transform it to the normal case?










share|cite|improve this question









$endgroup$



put on hold as off-topic by Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel Mar 11 at 14:01


This question appears to be off-topic. The users who voted to close gave this specific reason:


  • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel
If this question can be reworded to fit the rules in the help center, please edit the question.




















    0












    $begingroup$



    Solve
    $$begincases
    u_t-u_xx=frac12xt &textfor 0lt xlt pi, tgt0\
    u(0,t)=u(pi,t)=0 \
    u(x,0) = sin x \
    endcases$$




    How to transform it to the normal case?










    share|cite|improve this question









    $endgroup$



    put on hold as off-topic by Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel Mar 11 at 14:01


    This question appears to be off-topic. The users who voted to close gave this specific reason:


    • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel
    If this question can be reworded to fit the rules in the help center, please edit the question.


















      0












      0








      0





      $begingroup$



      Solve
      $$begincases
      u_t-u_xx=frac12xt &textfor 0lt xlt pi, tgt0\
      u(0,t)=u(pi,t)=0 \
      u(x,0) = sin x \
      endcases$$




      How to transform it to the normal case?










      share|cite|improve this question









      $endgroup$





      Solve
      $$begincases
      u_t-u_xx=frac12xt &textfor 0lt xlt pi, tgt0\
      u(0,t)=u(pi,t)=0 \
      u(x,0) = sin x \
      endcases$$




      How to transform it to the normal case?







      pde






      share|cite|improve this question













      share|cite|improve this question











      share|cite|improve this question




      share|cite|improve this question










      asked Mar 11 at 9:20









      Jaqen ChouJaqen Chou

      460110




      460110




      put on hold as off-topic by Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel Mar 11 at 14:01


      This question appears to be off-topic. The users who voted to close gave this specific reason:


      • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel
      If this question can be reworded to fit the rules in the help center, please edit the question.







      put on hold as off-topic by Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel Mar 11 at 14:01


      This question appears to be off-topic. The users who voted to close gave this specific reason:


      • "This question is missing context or other details: Please provide additional context, which ideally explains why the question is relevant to you and our community. Some forms of context include: background and motivation, relevant definitions, source, possible strategies, your current progress, why the question is interesting or important, etc." – Eevee Trainer, Cesareo, Gibbs, José Carlos Santos, Parcly Taxel
      If this question can be reworded to fit the rules in the help center, please edit the question.




















          1 Answer
          1






          active

          oldest

          votes


















          1












          $begingroup$

          Try to find a solution of the form



          $$ u(x,t) = sum_n T_n(t)X_n(x) $$



          where



          begincases
          X'' = -lambda^2 X \
          X(0) = X(pi) = 0
          endcases



          You'll get



          $$ u(x,t) = sum_n=1^infty T_n(t)sin(nx) $$



          and the PDE becomes



          $$ sum_n=1^inftybig[T_n'(t) + n^2T_n(t)big]sin(nx) = frac12 tx $$



          Decompose the RHS into the corresponding Fourier series



          $$ frac12 tx = sum_n=1^infty a_n(t) sin(nx) $$



          You'll get a family of IVPs



          begincases
          T_n''(t) + n^2 T_n(t) = a_n(t) \
          T_1(0) = 1 \
          T_n>1(0) = 0
          endcases






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:45










          • $begingroup$
            The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
            $endgroup$
            – Dylan
            Mar 11 at 10:51










          • $begingroup$
            Okay, think I'll find it in my following study. Thanks a lot
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:55

















          1 Answer
          1






          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          1












          $begingroup$

          Try to find a solution of the form



          $$ u(x,t) = sum_n T_n(t)X_n(x) $$



          where



          begincases
          X'' = -lambda^2 X \
          X(0) = X(pi) = 0
          endcases



          You'll get



          $$ u(x,t) = sum_n=1^infty T_n(t)sin(nx) $$



          and the PDE becomes



          $$ sum_n=1^inftybig[T_n'(t) + n^2T_n(t)big]sin(nx) = frac12 tx $$



          Decompose the RHS into the corresponding Fourier series



          $$ frac12 tx = sum_n=1^infty a_n(t) sin(nx) $$



          You'll get a family of IVPs



          begincases
          T_n''(t) + n^2 T_n(t) = a_n(t) \
          T_1(0) = 1 \
          T_n>1(0) = 0
          endcases






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:45










          • $begingroup$
            The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
            $endgroup$
            – Dylan
            Mar 11 at 10:51










          • $begingroup$
            Okay, think I'll find it in my following study. Thanks a lot
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:55















          1












          $begingroup$

          Try to find a solution of the form



          $$ u(x,t) = sum_n T_n(t)X_n(x) $$



          where



          begincases
          X'' = -lambda^2 X \
          X(0) = X(pi) = 0
          endcases



          You'll get



          $$ u(x,t) = sum_n=1^infty T_n(t)sin(nx) $$



          and the PDE becomes



          $$ sum_n=1^inftybig[T_n'(t) + n^2T_n(t)big]sin(nx) = frac12 tx $$



          Decompose the RHS into the corresponding Fourier series



          $$ frac12 tx = sum_n=1^infty a_n(t) sin(nx) $$



          You'll get a family of IVPs



          begincases
          T_n''(t) + n^2 T_n(t) = a_n(t) \
          T_1(0) = 1 \
          T_n>1(0) = 0
          endcases






          share|cite|improve this answer









          $endgroup$












          • $begingroup$
            There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:45










          • $begingroup$
            The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
            $endgroup$
            – Dylan
            Mar 11 at 10:51










          • $begingroup$
            Okay, think I'll find it in my following study. Thanks a lot
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:55













          1












          1








          1





          $begingroup$

          Try to find a solution of the form



          $$ u(x,t) = sum_n T_n(t)X_n(x) $$



          where



          begincases
          X'' = -lambda^2 X \
          X(0) = X(pi) = 0
          endcases



          You'll get



          $$ u(x,t) = sum_n=1^infty T_n(t)sin(nx) $$



          and the PDE becomes



          $$ sum_n=1^inftybig[T_n'(t) + n^2T_n(t)big]sin(nx) = frac12 tx $$



          Decompose the RHS into the corresponding Fourier series



          $$ frac12 tx = sum_n=1^infty a_n(t) sin(nx) $$



          You'll get a family of IVPs



          begincases
          T_n''(t) + n^2 T_n(t) = a_n(t) \
          T_1(0) = 1 \
          T_n>1(0) = 0
          endcases






          share|cite|improve this answer









          $endgroup$



          Try to find a solution of the form



          $$ u(x,t) = sum_n T_n(t)X_n(x) $$



          where



          begincases
          X'' = -lambda^2 X \
          X(0) = X(pi) = 0
          endcases



          You'll get



          $$ u(x,t) = sum_n=1^infty T_n(t)sin(nx) $$



          and the PDE becomes



          $$ sum_n=1^inftybig[T_n'(t) + n^2T_n(t)big]sin(nx) = frac12 tx $$



          Decompose the RHS into the corresponding Fourier series



          $$ frac12 tx = sum_n=1^infty a_n(t) sin(nx) $$



          You'll get a family of IVPs



          begincases
          T_n''(t) + n^2 T_n(t) = a_n(t) \
          T_1(0) = 1 \
          T_n>1(0) = 0
          endcases







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Mar 11 at 10:08









          DylanDylan

          13.9k31027




          13.9k31027











          • $begingroup$
            There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:45










          • $begingroup$
            The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
            $endgroup$
            – Dylan
            Mar 11 at 10:51










          • $begingroup$
            Okay, think I'll find it in my following study. Thanks a lot
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:55
















          • $begingroup$
            There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:45










          • $begingroup$
            The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
            $endgroup$
            – Dylan
            Mar 11 at 10:51










          • $begingroup$
            Okay, think I'll find it in my following study. Thanks a lot
            $endgroup$
            – Jaqen Chou
            Mar 11 at 10:55















          $begingroup$
          There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
          $endgroup$
          – Jaqen Chou
          Mar 11 at 10:45




          $begingroup$
          There is one thing I'm confused, in fact we can get $X''=-lambda^2 X$ in homogeneous case because $fracX''X=fracT'T$ has to be a constant. But in this nonhomogeneous case, I can only get $T'X=X''T+frac12xt$.
          $endgroup$
          – Jaqen Chou
          Mar 11 at 10:45












          $begingroup$
          The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
          $endgroup$
          – Dylan
          Mar 11 at 10:51




          $begingroup$
          The full explanation is a bit complicated. This method isn't separation of variables, just related to it. It just so happens that the eigenfunctions in $x$ span the full function space, so we use it as a basis of our solution. Think of it like an eigenvalue-eigenvector decomposition.
          $endgroup$
          – Dylan
          Mar 11 at 10:51












          $begingroup$
          Okay, think I'll find it in my following study. Thanks a lot
          $endgroup$
          – Jaqen Chou
          Mar 11 at 10:55




          $begingroup$
          Okay, think I'll find it in my following study. Thanks a lot
          $endgroup$
          – Jaqen Chou
          Mar 11 at 10:55



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