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Next: III. Up: Heat equation. Fourier method Previous: I.

II. $\lambda = 0.$

The general solution for (1.2) is

\begin{displaymath}
G(x) = C_1 x + C_2
\end{displaymath}

The boundary conditions

\begin{displaymath}
G(0) = 0,\;\; G(L) = 0
\end{displaymath}

imply that

\begin{displaymath}
C_2 = 0 \mbox{ follows from } G(0)=0
\end{displaymath}

and

\begin{displaymath}
C_1 L = 0 \mbox{ follows from } G(L) = 0
\end{displaymath}

Hence, the only possible solution is $C_1=0$ and $C_2=0.$



Sergey Nikitin 2004-10-25