Galerkin method

Inmathematics,in the area ofnumerical analysis,Galerkin methodsare a family of methods for converting a continuous operator problem, such as adifferential equation,commonly in aweak formulation,to a discrete problem by applying linear constraints determined by finite sets of basis functions. They are named after the Soviet mathematicianBoris Galerkin.

Often when referring to a Galerkin method, one also gives the name along with typical assumptions and approximation methods used:

• Ritz–Galerkin method(afterWalther Ritz) typically assumessymmetricandpositive definitebilinear formin theweak formulation,where thedifferential equationfor aphysical systemcan be formulated viaminimizationof aquadratic functionrepresenting the systemenergyand the approximate solution is alinear combinationof the given set of the basis functions.
• Bubnov–Galerkin method(afterIvan Bubnov) does not require thebilinear formto besymmetricand substitutes the energy minimization withorthogonalityconstraints determined by the same basis functions that are used to approximate the solution. In an operator formulation of thedifferential equation,Bubnov–Galerkin method can be viewed as applying anorthogonal projectionto the operator.
• Petrov–Galerkin method(afterGeorgii I. Petrov) allows using basis functions for orthogonality constraints (calledtest basis functions) that are different from the basis functions used to approximate the solution. Petrov–Galerkin method can be viewed as an extension of Bubnov–Galerkin method, applying a projection that is not necessarily orthogonal in the operator formulation of thedifferential equation.

Examples of Galerkin methods are:

• theGalerkin method of weighted residuals,the most common method of calculating the globalstiffness matrixin thefinite element method,
• theboundary element methodfor solving integral equations,
• Krylov subspace methods.

Example: Matrix linear system

We first introduce and illustrate the Galerkin method as being applied to a system of linear equations$A\mathbf {x} =\mathbf {b}$.We define the parameters as follow:

$A={\begin{bmatrix}2&0&0\\0&2&1\\0&1&2\end{bmatrix}}$

which is symmetric and positive definite, and the right-hand-side

$\mathbf {b} ={\begin{bmatrix}2\\0\\0\end{bmatrix}}.$

The true solution to this linear system is

$\mathbf {x} ={\begin{bmatrix}1\\0\\0\end{bmatrix}}.$

With Galerkin method, we can solve the system in a lower-dimensional space to obtain an approximate solution. Let us use the following basis for the subspace:

$V={\begin{bmatrix}0&0\\1&0\\0&1\end{bmatrix}}.$

Then, we can write the Galerkin equation$\left(V^{*}AV\right)\mathbf {y} =V^{*}\mathbf {b}$where the left-hand-side matrix is

$V^{*}AV={\begin{bmatrix}2&1\\1&2\end{bmatrix}},$

and the right-hand-side vector is

$V^{*}\mathbf {b} ={\begin{bmatrix}0\\0\end{bmatrix}}.$

We can then obtain the solution vector in the subspace:

$\mathbf {y} ={\begin{bmatrix}0\\0\end{bmatrix}},$

which we finally project back to the original space to determine the approximate solution to the original equation as

$V\mathbf {y} ={\begin{bmatrix}0\\0\\0\end{bmatrix}}.$

In this example, our originalHilbert spaceis actually the 3-dimensional Euclidean space$\mathbb {R} ^{3}$equipped with the standard scalar product$(\mathbf {u},\mathbf {v} )=\mathbf {u} ^{T}\mathbf {v}$,our 3-by-3 matrix$A$defines thebilinear form$a(\mathbf {u},\mathbf {v} )=\mathbf {u} ^{T}A\mathbf {v}$,and the right-hand-side vector$\mathbf {b}$defines thebounded linear functional$f(\mathbf {v} )=\mathbf {b} ^{T}\mathbf {v}$.The columns

$\mathbf {e} _{1}={\begin{bmatrix}0\\1\\0\end{bmatrix}}\quad \mathbf {e} _{2}={\begin{bmatrix}0\\0\\1\end{bmatrix}},$

of the matrix$V$form an orthonormal basis of the 2-dimensional subspace of the Galerkin projection. The entries of the 2-by-2 Galerkin matrix$V^{*}AV$are$a(e_{j},e_{i}),\,i,j=1,2$,while the components of the right-hand-side vector$V^{*}\mathbf {b}$of the Galerkin equation are$f(e_{i}),\,i=1,2$.Finally, the approximate solution$V\mathbf {y}$is obtained from the components of the solution vector$\mathbf {y}$of the Galerkin equation and the basis as$\sum _{j=1}^{2}y_{j}\mathbf {e} _{j}$.

Linear equation in a Hilbert space

Weak formulation of a linear equation

Let us introduce Galerkin's method with an abstract problem posed as aweak formulationon aHilbert space$V$,namely,

find$u\in V$such that for all$v\in V,a(u,v)=f(v)$.

Here,$a(\cdot,\cdot )$is abilinear form(the exact requirements on$a(\cdot,\cdot )$will be specified later) and$f$is a bounded linear functional on$V$.

Galerkin dimension reduction

Choose a subspace$V_{n}\subset V$of dimensionnand solve the projected problem:

Find$u_{n}\in V_{n}$such that for all$v_{n}\in V_{n},a(u_{n},v_{n})=f(v_{n})$.

We call this theGalerkin equation.Notice that the equation has remained unchanged and only the spaces have changed. Reducing the problem to a finite-dimensional vector subspace allows us to numerically compute$u_{n}$as a finite linear combination of the basis vectors in$V_{n}$.

Galerkin orthogonality

The key property of the Galerkin approach is that the error is orthogonal to the chosen subspaces. Since$V_{n}\subset V$,we can use$v_{n}$as a test vector in the original equation. Subtracting the two, we get the Galerkin orthogonality relation for the error,$\epsilon _{n}=u-u_{n}$which is the error between the solution of the original problem,$u$,and the solution of the Galerkin equation,$u_{n}$

$a(\epsilon _{n},v_{n})=a(u,v_{n})-a(u_{n},v_{n})=f(v_{n})-f(v_{n})=0.$

Matrix form of Galerkin's equation

Since the aim of Galerkin's method is the production of alinear system of equations,we build its matrix form, which can be used to compute the solution algorithmically.

Let$e_{1},e_{2},\ldots,e_{n}$be abasisfor$V_{n}$.Then, it is sufficient to use these in turn for testing the Galerkin equation, i.e.: find$u_{n}\in V_{n}$such that

$a(u_{n},e_{i})=f(e_{i})\quad i=1,\ldots,n.$

We expand$u_{n}$with respect to this basis,$u_{n}=\sum _{j=1}^{n}u_{j}e_{j}$and insert it into the equation above, to obtain

$a\left(\sum _{j=1}^{n}u_{j}e_{j},e_{i}\right)=\sum _{j=1}^{n}u_{j}a(e_{j},e_{i})=f(e_{i})\quad i=1,\ldots,n.$

This previous equation is actually a linear system of equations$Au=f$,where

$A_{ij}=a(e_{j},e_{i}),\quad f_{i}=f(e_{i}).$

Symmetry of the matrix

Due to the definition of the matrix entries, the matrix of the Galerkin equation issymmetricif and only if the bilinear form$a(\cdot,\cdot )$is symmetric.

Analysis of Galerkin methods

Here, we will restrict ourselves to symmetricbilinear forms,that is

$a(u,v)=a(v,u).$

While this is not really a restriction of Galerkin methods, the application of the standard theory becomes much simpler. Furthermore, aPetrov–Galerkin methodmay be required in the nonsymmetric case.

The analysis of these methods proceeds in two steps. First, we will show that the Galerkin equation is awell-posed problemin the sense ofHadamardand therefore admits a unique solution. In the second step, we study the quality of approximation of the Galerkin solution$u_{n}$.

The analysis will mostly rest on two properties of thebilinear form,namely

• Boundedness: for all$u,v\in V$holds

  $a(u,v)\leq C\|u\|\,\|v\|$for some constant$C>0$

• Ellipticity: for all$u\in V$holds

  $a(u,u)\geq c\|u\|^{2}$for some constant$c>0.$

By the Lax-Milgram theorem (seeweak formulation), these two conditions imply well-posedness of the original problem in weak formulation. All norms in the following sections will be norms for which the above inequalities hold (these norms are often called an energy norm).

Well-posedness of the Galerkin equation

Since$V_{n}\subset V$,boundedness and ellipticity of the bilinear form apply to$V_{n}$.Therefore, the well-posedness of the Galerkin problem is actually inherited from the well-posedness of the original problem.

Quasi-best approximation (Céa's lemma)

Main article:Céa's lemma

The error$u-u_{n}$between the original and the Galerkin solution admits the estimate

$\|u-u_{n}\|\leq {\frac {C}{c}}\inf _{v_{n}\in V_{n}}\|u-v_{n}\|.$

This means, that up to the constant$C/c$,the Galerkin solution$u_{n}$ is as close to the original solution$u$as any other vector in$V_{n}$.In particular, it will be sufficient to study approximation by spaces$V_{n}$,completely forgetting about the equation being solved.

Proof

Since the proof is very simple and the basic principle behind all Galerkin methods, we include it here: by ellipticity and boundedness of the bilinear form (inequalities) and Galerkin orthogonality (equals sign in the middle), we have for arbitrary$v_{n}\in V_{n}$:

$c\|u-u_{n}\|^{2}\leq a(u-u_{n},u-u_{n})=a(u-u_{n},u-v_{n})\leq C\|u-u_{n}\|\,\|u-v_{n}\|.$

Dividing by$c\|u-u_{n}\|$and taking the infimum over all possible$v_{n}$yields the lemma.

Galerkin's best approximation property in the energy norm

For simplicity of presentation in the section above we have assumed that the bilinear form$a(u,v)$is symmetric and positive definite, which implies that it is ascalar productand the expression$\|u\|_{a}={\sqrt {a(u,u)}}$is actually a valid vector norm, called theenergy norm.Under these assumptions one can easily prove in addition Galerkin's best approximation property in the energy norm.

Using Galerkin a-orthogonality and theCauchy–Schwarz inequalityfor the energy norm, we obtain

$\|u-u_{n}\|_{a}^{2}=a(u-u_{n},u-u_{n})=a(u-u_{n},u-v_{n})\leq \|u-u_{n}\|_{a}\,\|u-v_{n}\|_{a}.$

Dividing by$\|u-u_{n}\|_{a}$and taking the infimum over all possible$v_{n}\in V_{n}$proves that the Galerkin approximation$u_{n}\in V_{n}$is the best approximation in the energy norm within the subspace$V_{n}\subset V$,i.e.$u_{n}\in V_{n}$is nothing but the orthogonal, with respect to thescalar product$a(u,v)$,projection of the solution$u$to the subspace$V_{n}$.

Galerkin method for stepped Structures

I. Elishakof,M. Amato, A. Marzani, P.A. Arvan, and J.N. Reddy studied the application of the Galerkin method to stepped structures. They showed that the generalized function, namely unit-step function, Dirac’s delta function, and the doublet function are needed for obtaining accurate results.

History

The approach is usually credited toBoris Galerkin.The method was explained to the Western reader by Henckyand Duncanamong others. Its convergence was studied by Mikhlinand LeipholzIts coincidence with Fourier method was illustrated byElishakoffet al.Its equivalence to Ritz's method for conservative problems was shown by Singer.Gander and Wannershowed how Ritz and Galerkin methods led to the modern finite element method. One hundred years of method's development was discussed by Repin.Elishakoff, Kaplunov and Kaplunovshow that the Galerkin’s method was not developed by Ritz, contrary to the Timoshenko’s statements.

See also

• Ritz method

External links

• "Galerkin method",Encyclopedia of Mathematics,EMS Press,2001 [1994]
• Galerkin Method from MathWorld