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Difference between revisions of "Reduced Basis PMOR method"

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<math> V_1 \subset V_2 \subset ... \subset V_{N_{max}} </math>.
 
<math> V_1 \subset V_2 \subset ... \subset V_{N_{max}} </math>.
  +
  +
We then consider the galerkin projection onto the RB-space <math> V_N </math>
  +
  +
<math>
  +
\begin{cases}
  +
\text{For } \mu \in \mathcal{D} \subset \mathbb{R}^P, \text{ evaluate } \\
  +
s_N^\mathcal{N}(\mu) = f(u_N^\mathcal{N}(\mu)), \\
  +
\text{where } u_N^\mathcal{N}(\mu) \in W_N^\mathcal{N} \text{ satisfies } \\
  +
a(u_N^\mathcal{N}(\mu),v;\mu) = f(v), \forall v \in W_N^\mathcal{N}
  +
\end{cases}
  +
</math>
   
 
==Time-Dependent PDEs==
 
==Time-Dependent PDEs==

Revision as of 16:33, 19 November 2012


The Reduced Basis Method (RBM) we present here is applicable to static and time-dependent linear PDEs.

Time-Independent PDEs

The typical model problem of the RBM consists of a parametrized PDE stated in weak form with bilinear form  a(\cdot, \cdot; \mu) and linear form  f(\cdot; \mu) . The parameter  \mu is considered within a domain  \mathcal{D} and we are interested in an output quantity  s(\mu) which can be expressed via a linear functional of the field variable  l(\cdot; \mu) .

The exact, infinite-dimensional formulation, indicated by the superscript e, is given by



\begin{cases}
\text{For } \mu \in \mathcal{D} \subset \mathbb{R}^P, \text{ evaluate } \\
s^e(\mu) = l(u^e(\mu);\mu), \\
\text{where } u^e(\mu) \in X^e(\Omega) \text{ satisfies } \\
a(u^e(\mu),v;\mu) = f(v;\mu), \forall v \in X^e.
\end{cases}

We assume a large-scale discretization to be given, such that we consider


\begin{cases}
\text{For } \mu \in \mathcal{D} \subset \mathbb{R}^P, \text{ evaluate } \\
s(\mu) = l(u(\mu);\mu), \\
\text{where } u(\mu) \in X(\Omega) \text{ satisfies } \\
a(u(\mu),v;\mu) = f(v;\mu), \forall v \in X.
\end{cases}

The underlying assumption of the RBM is that the parametrically induced manifold  \mathcal{M} = \{u(\mu) | \mu \in \mathcal{D}\} can be approximated by a low dimensional space  V_N .

It also applies the concept of an offline-online decomposition, in that a large pre-processing offline cost is acceptable in view of a very low online cost (of a reduced order model) for each input-output evaluation, when in a many-query or real-time context.

The essential assumption which allows the offline-online decomposition is that there exists an affine parameter dependence


 a(w,v;\mu) = \sum_{q=1}^Q \Theta_a^q(\mu) a^q(w,v)


 f(v;\mu) = \sum_{q=1}^{Q^f} \Theta_f^{q}(\mu) f^q(v).

The Lagrange Reduced Basis space is established by iteratively choosing Lagrange parameter samples

 
S_N = \{\mu^1,...,\mu^N\}

and considering the associated Lagrange RB spaces 

 
V_N = \text{span}\{u^\mathcal{N}(\mu^n), 1 \leq n \leq N \}

in a greedy sampling.
This leads to hierarchical RB spaces: 

 V_1 \subset V_2 \subset ... \subset V_{N_{max}} .

We then consider the galerkin projection onto the RB-space  V_N


\begin{cases}
\text{For } \mu \in \mathcal{D} \subset \mathbb{R}^P, \text{ evaluate } \\
s_N^\mathcal{N}(\mu) = f(u_N^\mathcal{N}(\mu)), \\
\text{where } u_N^\mathcal{N}(\mu) \in W_N^\mathcal{N} \text{ satisfies } \\
a(u_N^\mathcal{N}(\mu),v;\mu) = f(v), \forall v \in W_N^\mathcal{N}
\end{cases}

Time-Dependent PDEs

References