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Next: Consequences of a reordering Up: Mathematical properties of the Previous: Matrix form of the   Contents   Index

Mathematical properties expressed using the matrix form

The matrix form of the equations (1.58) making up the discretized multi-group diffusion equations is a generalized eigenvalue problem since we may rewrite the matrix equation as

\begin{displaymath}
\nu \hspace{0.2ex}\underline{\underline{F}}{}\hspace{0.15ex...
...hspace{0.15ex} \hspace{0.2ex}\underline{\Phi}{}\hspace{0.15ex}
\end{displaymath} (1.43)

We are now able to identify that we are in fact dealing with a generalized eigenvalue problem since $\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex} \ne \hspace{0.2ex}\underline{\underline{I}}{}\hspace{0.15ex}$.

We are, of course, able mathematically1.20 to write the generalized eigenvalue problem in a form which resembles a simple eigenvalue problem. This is shown below

\begin{displaymath}
\nu \hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex...
...x} = \lambda_0 \hspace{0.2ex}\underline{\Phi}{}\hspace{0.15ex}
\end{displaymath} (1.44)

Finally, we are able to state the theorems specifying the mathematical properties of the discretized multi-group diffusion equations

Theorem 1.1 (Cf. Wachspress [4])   The real parts of the eigenvalues of the matrix $\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex}$ are positive

\begin{displaymath}
Re[ \lambda(\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex})] > 0
\end{displaymath} (1.45)

and the matrix $\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex}$ has a non-negative inverse matrix $\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex}^{-1}$.

Theorem 1.2 (Cf. Wachspress [4])   There is a unique positive eigenvector of the matrix $\nu \hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex}^{-1}
\hspace{0.2ex}\underline{\underline{F}}{}\hspace{0.15ex}$, with real eigenvalue $\lambda_0$ greater in modulus than all other eigenvalues of matrix $\nu \hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex}^{-1}
\hspace{0.2ex}\underline{\underline{F}}{}\hspace{0.15ex}$.

Theorem 1.3 (Cf. Wachspress [4])   For $\lambda_e > 0$, the matrix $(\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex} - \frac{\nu}{\lambda_e}\hspace{0.2ex}\underline{\underline{F}}{}\hspace{0.15ex})$ has a non-negative inverse if and only if $\lambda_e > \lambda_0$.

Theorem 1.4 (Cf. Wachspress [4])   The inverse of any principal matrix minor1.21 of $(\hspace{0.2ex}\underline{\underline{B}}{}\hspace{0.15ex} -
\frac{\nu}{\lambda_e}\hspace{0.2ex}\underline{\underline{F}}{}\hspace{0.15ex})$ is non-negative for $\lambda_e >
\lambda_0$1.22.

Note that we in this mathematical treatment assume $\nu$ as being independent of energy--consequently we only have one $\nu$. This simplification is not by any means restrictive--the mathematical properties fit the situation of $\nu = \nu(E)$ as well since the energy dependence of $\nu$ only "perturbs" the $\overline{\Sigma}{}_{f,k}^g$'s slightly.


next up previous contents index
Next: Consequences of a reordering Up: Mathematical properties of the Previous: Matrix form of the   Contents   Index  
 
 
 
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