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In this case
does not exists and we
have a symbol
![$\displaystyle \hat{\cal H} (k_1) = \frac{k_1^2}{\vert 1- M^2 \vert }.$](img134.png) |
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(51) |
This is the symbol of the differential operator
![$\displaystyle - \frac{1}{\vert 1- M^2 \vert } \frac{\partial ^2 }{\partial x^2}.$](img135.png) |
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(52) |
A preconditioned gradient descent method have the form
![$\displaystyle \begin{array}{c}
\mu \psi - \frac{1}{\vert 1 - M^2 }\vert \frac{d...
...al \lambda }{\partial x} \\
\alpha \leftarrow \alpha - \delta \psi
\end{array}$](img136.png) |
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(53) |
That is, we have to solve an ODE on the boundary with the gradient as a source
term, before using it as a direction of change for the design variable.
According to our analysis the new method converges at a rate with
is independent of the number of design variables, since the symbol for
the modified iteration does not depend on
.
Note that the construction of the preconditioner was done on the differential
level but the numerical implementation is using some approximation of it, e.g.,
finite difference approximation.
Next: Three Dimensional Case
Up: Small Disturbance Potential Equation
Previous: Small Disturbance Potential Equation
Shlomo Ta'asan
2001-08-22