galerkin()

InterpConstantOperator.galerkin(Vr, Wr=None)

Project this operator to a low-dimensional linear space.

Consider an interpolatory operator

\[\f_\ell(\q,\u;\bfmu) = \textrm{interpolate}( (\bfmu_0,\f_{\ell}^{(0)}(\q,\u)),\ldots, (\bfmu_{s-1},\f_{\ell}^{(s-1)}(\q,\u)); \bfmu),\]

where

• \(\q\in\RR^n\) is the full-order state,

• \(\u\in\RR^m\) is the input,

• \(\bfmu_0,\ldots,\bfmu_{s-1}\in\RR^p\) are the (fixed) training parameter values,

• \(\f_{\ell}^{(i)}(\q,\u) = \f_{\ell}(\q,\u;\bfmu_i)\) is the operators evaluated at the \(i\)-th training parameter values, \(i=1,\ldots,s\), and

• \(\bfmu\in\RR^p\) is a new parameter value at which to evaluate the operator.

Given a trial basis \(\Vr\in\RR^{n\times r}\) and a test basis \(\Wr\in\RR^{n\times r}\), the corresponding intrusive projection of \(\f\) is the interpolatory operator

\[\fhat_{\ell}(\qhat,\u;\bfmu) = \textrm{interpolate}( (\bfmu_0,\Wr\trp\f_{\ell}^{(0)}(\Vr\qhat,\u)),\ldots, (\bfmu_{s-1},\Wr\trp\f_{\ell}^{(s-1)}(\Vr\qhat,\u)); \bfmu),\]

Here, \(\qhat\in\RR^r\) is the reduced-order state, which enables the low-dimensional state approximation \(\q = \Vr\qhat\). If \(\Wr = \Vr\), the result is called a Galerkin projection. If \(\Wr \neq \Vr\), it is called a Petrov-Galerkin projection.

Parameters:

Vr(n, r) ndarray

Basis for the trial space.

Wr(n, r) ndarray or None

Basis for the test space. If None, defaults to Vr.

Returns:

opoperator

New object of the same class as self.