Finite element method

 ( Continuum Mechanics ) 

Finite element method ( FEM) is a popular method for numerically solving differential equations arising in engineering and mathematical modeling. Typical problem areas of interest include the traditional fields of structural analysis, heat transfer, fluid flow, mass transport, and electromagnetic potential. Computers are usually used to perform the calculations required. With high-speed , better solutions can be achieved and are often required to solve the largest and most complex problems.

FEM is a general numerical method for solving partial differential equations in two- or three-space variables (i.e., some boundary value problems). There are also studies about using FEM to solve high-dimensional problems. To solve a problem, FEM subdivides a large system into smaller, simpler parts called finite elements. This is achieved by a particular space discretization in the space dimensions, which is implemented by the construction of a mesh of the object: the numerical domain for the solution that has a finite number of points. FEM formulation of a boundary value problem finally results in a system of algebraic equations. The method approximates the unknown function over the domain.

The simple equations that model these finite elements are then assembled into a larger system of equations that models the entire problem. FEM then approximates a solution by minimizing an associated error function via the calculus of variations.

Studying or Analysis a phenomenon with FEM is often referred to as finite element analysis (FEA).

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Basic concepts The subdivision of a whole domain into simpler parts has several advantages:

(2025). 9780071267618, McGraw-Hill. ISBN 9780071267618

• Accurate representation of complex geometry;
• Inclusion of dissimilar material properties;
• Easy representation of the total solution; and
• Capture of local effects.

A typical approach using the method involves the following steps:

1. Dividing the domain of the problem into a collection of subdomains, with each subdomain represented by a set of element equations for the original problem.
2. Systematically recombining all sets of element equations into a global system of equations for the final calculation.

The global system of equations uses known solution techniques and can be calculated from the of the original problem to obtain a numerical answer.

In the first step above, the element equations are simple equations that locally approximate the original complex equations to be studied, where the original equations are often partial differential equations (PDEs). To explain the approximation of this process, FEM is commonly introduced as a special case of the Galerkin method. The process, in mathematical language, is to construct an integral of the inner product of the residual and the ; then, set the integral to zero. In simple terms, it is a procedure that minimizes the approximation error by fitting trial functions into the PDE. The residual is the error caused by the trial functions, and the weight functions are polynomial approximation functions that project the residual. The process eliminates all the spatial derivatives from the PDE, thus approximating the PDE locally using the following:

• a set of algebraic equations for steady state problems; and
• a set of ordinary differential equations for transient state problems.

These equation sets are element equations. They are linear if the underlying PDE is linear and vice versa. Algebraic equation sets that arise in the steady-state problems are solved using numerical linear algebraic methods. In contrast, ordinary differential equation sets that occur in the transient problems are solved by numerical integrations using standard techniques such as Euler's method or the Runge–Kutta method.

In the second step above, a global system of equations is generated from the element equations by transforming coordinates from the subdomains' local nodes to the domain's global nodes. This spatial transformation includes appropriate orientation adjustments as applied in relation to the reference coordinate system. The process is often carried out using FEM software with coordinates data generated from the subdomains.

The practical application of FEM is known as finite element analysis (FEA). FEA, as applied in engineering, is a computational tool for performing engineering analysis. It includes the use of mesh generation techniques for dividing a complex system into smaller elements, as well as the use of software coded with a FEM algorithm. When applying FEA, the complex problem is usually a physical system with the underlying physics, such as the Euler–Bernoulli beam equation, the heat equation, or the Navier–Stokes equations, expressed in either PDEs or integral equations, while the divided, smaller elements of the complex problem represent different areas in the physical system.

FEA may be used for analyzing problems over complicated domains (e.g., cars and oil pipelines) when the domain changes (e.g., during a solid-state reaction with a moving boundary), when the desired precision varies over the entire domain, or when the solution lacks smoothness. FEA simulations provide a valuable resource, as they remove multiple instances of creating and testing complex prototypes for various high-fidelity situations. For example, in a frontal crash simulation, it is possible to increase prediction accuracy in important areas, like the front of the car, and reduce it in the rear of the car, thus reducing the cost of the simulation. Another example would be in numerical weather prediction, where it is more important to have accurate predictions over developing highly nonlinear phenomena, such as in the atmosphere or eddies in the ocean, rather than relatively calm areas.

A clear, detailed, and practical presentation of this approach can be found in the textbook The Finite Element Method for Engineers.

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History While it is difficult to quote the date of the invention of FEM, the method originated from the need to solve complex elasticity and structural analysis problems in civil and aeronautical engineering. Its development can be traced back to work by Alexander Hrennikoff and Richard Courant in the early 1940s. Another pioneer was Ioannis Argyris. In the USSR, the introduction of the practical application of FEM is usually connected with Leonard Oganesyan. It was also independently rediscovered in China by Feng Kang in the late 1950s and early 1960s, based on the computations of dam constructions, where it was called the "finite difference method" based on variation principles. Although the approaches used by these pioneers are different, they share one essential characteristic: the Polygon mesh discretization of a continuous domain into a set of discrete sub-domains, usually called elements.

Hrennikoff's work discretizes the domain by using a lattice analogy, while Courant's approach divides the domain into finite triangular sub-regions to solve second-order elliptic partial differential equations that arise from the problem of the torsion of a cylinder. Courant's contribution was evolutionary, drawing on a large body of earlier results for PDEs developed by Lord Rayleigh, Walther Ritz, and Boris Galerkin.

The application of FEM gained momentum in the 1960s and 1970s due to the developments of John Argyris and his co-workers at the University of Stuttgart; R. W. Clough and his co-workers at University of California Berkeley; O. C. Zienkiewicz and his co-workers Ernest Hinton, Bruce Irons, and others at Swansea University; Philippe G. Ciarlet at the University of Paris 6; and Richard Gallagher and his co-workers at Cornell University. During this period, additional impetus was provided by the available open-source FEM programs. NASA sponsored the original version of NASTRAN. University of California Berkeley made the finite element programs SAP IV and, later, OpenSees widely available. In Norway, the ship classification society Det Norske Veritas (now DNV GL) developed Sesam in 1969 for use in the analysis of ships.

A rigorous mathematical basis for FEM was provided in 1973 with a publication by Gilbert Strang and George Fix.

(1973). 9780130329462, Prentice Hall. . ISBN 9780130329462

The method has since been generalized for the numerical modeling of physical systems in a wide variety of engineering disciplines, such as electromagnetism, heat transfer, and fluid dynamics.

(2013). 9780080951355, Butterworth-Heinemann. . ISBN 9780080951355

(2025). 9780979004902, Cambridge, MA: Klaus-Jürgen Bathe. ISBN 9780979004902

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Technical discussion

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The structure of finite element methods A finite element method is characterized by a variational formulation, a discretization strategy, one or more solution algorithms, and post-processing procedures.

Examples of the variational formulation are the Galerkin method, the discontinuous Galerkin method, mixed methods, etc.

A discretization strategy is understood to mean a clearly defined set of procedures that cover (a) the creation of finite element meshes, (b) the definition of basis function on reference elements (also called shape functions), and (c) the mapping of reference elements onto the elements of the mesh. Examples of discretization strategies are the h-version, p-FEM, Hp-FEM, x-FEM, isogeometric analysis, etc. Each discretization strategy has certain advantages and disadvantages. A reasonable criterion in selecting a discretization strategy is to realize nearly optimal performance for the broadest set of mathematical models in a particular model class.

Various numerical solution algorithms can be classified into two broad categories; direct and iterative solvers. These algorithms are designed to exploit the sparsity of matrices that depend on the variational formulation and discretization strategy choices.

Post-processing procedures are designed to extract the data of interest from a finite element solution. To meet the requirements of solution verification, postprocessors need to provide for a posteriori error estimation in terms of the quantities of interest. When the errors of approximation are larger than what is considered acceptable, then the discretization has to be changed either by an automated adaptive process or by the action of the analyst. Some very efficient postprocessors provide for the realization of superconvergence.

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Illustrative problems P1 and P2 The following two problems demonstrate the finite element method.

P1 is a one-dimensional problem $$\backslash text\{\; P1\; \}\; :\; \backslash begin\{cases\}\; u\text{'}\text{'}(x)\; =\; f(x)\; \backslash text\{\; in\; \}\; (0,1),\; \backslash \backslash \; u(0)\; =\; u(1)\; =\; 0,\; \backslash end\{cases\}$$ where $f$ is given, $u$ is an unknown function of $x$, and $u\text{'}\text{'}$ is the second derivative of $u$ with respect to $x$.

P2 is a two-dimensional problem (Dirichlet problem)

where $\backslash Omega$ is a connected open region in the $(x,y)$ plane whose boundary $\backslash partial\; \backslash Omega$ is nice (e.g., a smooth manifold or a polygon), and $u\_\{xx\}$ and $u\_\{yy\}$ denote the second derivatives with respect to $x$ and $y$, respectively.

The problem P1 can be solved directly by computing . However, this method of solving the boundary value problem (BVP) works only when there is one spatial dimension. It does not generalize to higher-dimensional problems or problems like $u+V\text{'}\text{'}=f$. For this reason, we will develop the finite element method for P1 and outline its generalization to P2.

Our explanation will proceed in two steps, which mirror two essential steps one must take to solve a boundary value problem (BVP) using the FEM.

• In the first step, one rephrases the original BVP in its weak form. Little to no computation is usually required for this step. The transformation is done by hand on paper.
• The second step is discretization, where the weak form is discretized in a finite-dimensional space.

After this second step, we have concrete formulae for a large but finite-dimensional linear problem whose solution will approximately solve the original BVP. This finite-dimensional problem is then implemented on a computer.

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Weak formulation The first step is to convert P1 and P2 into their equivalent .

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The weak form of P1 If $u$ solves P1, then for any smooth function $v$ that satisfies the displacement boundary conditions, i.e. $v=0$ at $x=0$ and $x=1$, we have

Conversely, if $u$ with $u(0)\; =\; u(1)\; =\; 0$ satisfies (1) for every smooth function $v(x)$ then one may show that this $u$ will solve P1. The proof is easier for twice continuously differentiable $u$ (mean value theorem) but may be proved in a distributional sense as well.

We define a new operator or map $\backslash phi(u,v)$ by using integration by parts on the right-hand-side of (1):

where we have used the assumption that $v(0)\; =\; v(1)\; =\; 0$.

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The weak form of P2 If we integrate by parts using a form of Green's identities, we see that if $u$ solves P2, then we may define $\backslash phi(u,v)$ for any $v$ by $$\backslash int\_\backslash Omega\; fv\backslash ,ds\; =\; -\backslash int\_\backslash Omega\; \backslash nabla\; u\; \backslash cdot\; \backslash nabla\; v\; \backslash ,\; ds\; \backslash equiv\; -\backslash phi(u,v),$$

where $\backslash nabla$ denotes the gradient and $\backslash cdot$ denotes the dot product in the two-dimensional plane. Once more $\backslash ,\backslash !\backslash phi$ can be turned into an inner product on a suitable space $H\_0^1(\backslash Omega)$ of once differentiable functions of $\backslash Omega$ that are zero on $\backslash partial\; \backslash Omega$. We have also assumed that $v\; \backslash in\; H\_0^1(\backslash Omega)$ (see ). The existence and uniqueness of the solution can also be shown.

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A proof outline of the existence and uniqueness of the solution We can loosely think of $H\_0^1(0,1)$ to be the absolutely continuous functions of $(0,1)$ that are $0$ at $x=0$ and $x=1$ (see Sobolev spaces). Such functions are (weakly) once differentiable, and it turns out that the symmetric bilinear map $\backslash !\backslash ,\backslash phi$ then defines an inner product which turns $H\_0^1(0,1)$ into a Hilbert space (a detailed proof is nontrivial). On the other hand, the left-hand-side $\backslash int\_0^1\; f(x)v(x)dx$ is also an inner product, this time on the Lp space $L^2(0,1)$. An application of the Riesz representation theorem for Hilbert spaces shows that there is a unique $u$ solving (2) and, therefore, P1. This solution is a-priori only a member of $H\_0^1(0,1)$, but using elliptic regularity, will be smooth if $f$ is.

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Discretization P1 and P2 are ready to be discretized, which leads to a common sub-problem (3). The basic idea is to replace the infinite-dimensional linear problem:

Find $u\; \backslash in\; H\_0^1$ such that

$\backslash forall\; v\; \backslash in\; H\_0^1,\; \backslash ;\; -\backslash phi(u,v)=\backslash int\; fv$

with a finite-dimensional version:

where $V$ is a finite-dimensional Linear subspace of $H\_0^1$. There are many possible choices for $V$ (one possibility leads to the spectral method). However, we take $V$ as a space of piecewise polynomial functions for the finite element method.

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For problem P1 We take the interval $(0,1)$, choose $n$ values of $x$ with and we define $V$ by: $$V\; =\; \backslash \{v:0,1\; \backslash to\; \backslash mathbb\; R\backslash ;:\; v\backslash text\{\; is\; continuous,\; \}\; v|\_\{x\_k,x\_\{k+1\}\}\; \backslash text\{\; is\; linear\; for\; \}\; k\; =\; 0,\backslash dots,n\; \backslash text\{,\; and\; \}\; v(0)=v(1)=0\; \backslash \}$$

where we define $x\_0=0$ and $x\_\{n+1\}=1$. Observe that functions in $V$ are not differentiable according to the elementary definition of calculus. Indeed, if $v\; \backslash in\; V$ then the derivative is typically not defined at any $x\; =\; x\_k$, $k\; =\; 1,\backslash ldots,n$. However, the derivative exists at every other value of $x$, and one can use this derivative for integration by parts.

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For problem P2 We need $V$ to be a set of functions of $\backslash Omega$. In the figure on the right, we have illustrated a triangulation of a 15-sided region $\backslash Omega$ in the plane (below), and a piecewise linear function (above, in color) of this polygon which is linear on each triangle of the triangulation; the space $V$ would consist of functions that are linear on each triangle of the chosen triangulation.

One hopes that as the underlying triangular mesh becomes finer and finer, the solution of the discrete problem (3) will, in some sense, converge to the solution of the original boundary value problem P2. To measure this mesh fineness, the triangulation is indexed by a real-valued parameter $h\; >\; 0$ which one takes to be very small. This parameter will be related to the largest or average triangle size in the triangulation. As we refine the triangulation, the space of piecewise linear functions $V$ must also change with $h$. For this reason, one often reads $V\_h$ instead of $V$ in the literature. Since we do not perform such an analysis, we will not use this notation.

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Choosing a basis To complete the discretization, we must select a basis of $V$. In the one-dimensional case, for each control point $x\_k$ we will choose the piecewise linear function $v\_k$ in $V$ whose value is $1$ at $x\_k$ and zero at every $x\_j,\backslash ;j\; \backslash neq\; k$, i.e.,

for $k\; =\; 1,\backslash dots,n$; this basis is a shifted and scaled tent function. For the two-dimensional case, we choose again one basis function $v\_k$ per vertex $x\_k$ of the triangulation of the planar region $\backslash Omega$. The function $v\_k$ is the unique function of $V$ whose value is $1$ at $x\_k$ and zero at every $x\_j,\backslash ;j\; \backslash neq\; k$.

Depending on the author, the word "element" in the "finite element method" refers to the domain's triangles, the piecewise linear basis function, or both. So, for instance, an author interested in curved domains might replace the triangles with curved primitives and so might describe the elements as being curvilinear. On the other hand, some authors replace "piecewise linear" with "piecewise quadratic" or even "piecewise polynomial". The author might then say "higher order element" instead of "higher degree polynomial". The finite element method is not restricted to triangles (tetrahedra in 3-d or higher-order simplexes in multidimensional spaces). Still, it can be defined on quadrilateral subdomains (hexahedra, prisms, or pyramids in 3-d, and so on). Higher-order shapes (curvilinear elements) can be defined with polynomial and even non-polynomial shapes (e.g., ellipse or circle).

Examples of methods that use higher degree piecewise polynomial basis functions are the hp-FEM and spectral FEM.

More advanced implementations (adaptive finite element methods) utilize a method to assess the quality of the results (based on error estimation theory) and modify the mesh during the solution aiming to achieve an approximate solution within some bounds from the exact solution of the continuum problem. Mesh adaptivity may utilize various techniques; the most popular are:

• moving nodes (r-adaptivity)
• refining (and unrefined) elements (h-adaptivity)
• changing order of base functions (p-adaptivity)
• combinations of the above (hp-FEM).

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Small support of the basis The primary advantage of this choice of basis is that the inner products $$\backslash langle\; v\_j,v\_k\; \backslash rangle\; =\; \backslash int\_0^1\; v\_j\; v\_k\backslash ,dx$$ and $$\backslash phi(v\_j,v\_k)=\backslash int\_0^1\; v\_j\text{'}\; v\_k\text{'}\backslash ,dx$$ will be zero for almost all $j,k$. (The matrix containing $\backslash langle\; v\_j,\; v\_k\; \backslash rangle$ in the $(j,k)$ location is known as the Gramian matrix.) In the one dimensional case, the support of $v\_k$ is the interval $x\_\{k-1\},x\_\{k+1\}$. Hence, the integrands of $\backslash langle\; v\_j,\; v\_k\; \backslash rangle$ and $\backslash phi(v\_j,v\_k)$ are identically zero whenever $|j-k|>1$.

Similarly, in the planar case, if $x\_j$ and $x\_k$ do not share an edge of the triangulation, then the integrals $$\backslash int\_\{\backslash Omega\}\; v\_j\; v\_k\backslash ,ds$$ and $$\backslash int\_\{\backslash Omega\}\; \backslash nabla\; v\_j\; \backslash cdot\; \backslash nabla\; v\_k\backslash ,ds$$ are both zero.

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Matrix form of the problem If we write $u(x)\; =\; \backslash sum\_\{k=1\}^n\; u\_k\; v\_k(x)$ and $f(x)\; =\; \backslash sum\_\{k=1\}^n\; f\_k\; v\_k(x)$ then problem (3), taking $v(x)\; =\; v\_j(x)$ for $j\; =\; 1,\; \backslash dots,\; n$, becomes

If we denote by $\backslash mathbf\{u\}$ and $\backslash mathbf\{f\}$ the column vectors $(u\_1,\backslash dots,u\_n)^t$ and $(f\_1,\backslash dots,f\_n)^t$, and if we let $$L\; =\; (L\_\{ij\})$$ and $$M\; =\; (M\_\{ij\})$$ be matrices whose entries are $$L\_\{ij\}\; =\; \backslash phi\; (v\_i,v\_j)$$ and $$M\_\{ij\}\; =\; \backslash int\; v\_i\; v\_j\; dx$$ then we may rephrase (4) as

It is not necessary to assume $f(x)\; =\; \backslash sum\_\{k=1\}^n\; f\_k\; v\_k(x)$. For a general function $f(x)$, problem (3) with $v(x)\; =\; v\_j(x)$ for $j\; =\; 1,\; \backslash dots,\; n$ becomes actually simpler, since no matrix $M$ is used,

where $\backslash mathbf\{b\}\; =\; (b\_1,\; \backslash dots,\; b\_n)^t$ and $b\_j\; =\; \backslash int\; f\; v\_j\; dx$ for $j\; =\; 1,\; \backslash dots,\; n$.

As we have discussed before, most of the entries of $L$ and $M$ are zero because the basis functions $v\_k$ have small support. So we now have to solve a linear system in the unknown $\backslash mathbf\{u\}$ where most of the entries of the matrix $L$, which we need to invert, are zero.

Such matrices are known as sparse matrix, and there are efficient solvers for such problems (much more efficient than actually inverting the matrix.) In addition, $L$ is symmetric and positive definite, so a technique such as the conjugate gradient method is favored. For problems that are not too large, sparse and Cholesky decompositions still work well. For instance, MATLAB's backslash operator (which uses sparse LU, sparse Cholesky, and other factorization methods) can be sufficient for meshes with a hundred thousand vertices.

The matrix $L$ is usually referred to as the stiffness matrix, while the matrix $M$ is dubbed the mass matrix.

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General form of the finite element method In general, the finite element method is characterized by the following process.

• One chooses a grid for $\backslash Omega$. In the preceding treatment, the grid consisted of triangles, but one can also use squares or curvilinear polygons.
• Then, one chooses basis functions. We used piecewise linear basis functions in our discussion, but it is common to use piecewise polynomial basis functions.

Separate consideration is the smoothness of the basis functions. For second-order elliptic boundary value problems, piecewise polynomial basis function that is merely continuous suffice (i.e., the derivatives are discontinuous.) For higher-order partial differential equations, one must use smoother basis functions. For instance, for a fourth-order problem such as $u\_\{xxxx\}\; +\; u\_\{yyyy\}\; =\; f$, one may use piecewise quadratic basis functions that are $C^1$.

Another consideration is the relation of the finite-dimensional space $V$ to its infinite-dimensional counterpart in the examples above $H\_0^1$. A conforming element method is one in which space $V$ is a subspace of the element space for the continuous problem. The example above is such a method. If this condition is not satisfied, we obtain a nonconforming element method, an example of which is the space of piecewise linear functions over the mesh, which are continuous at each edge midpoint. Since these functions are generally discontinuous along the edges, this finite-dimensional space is not a subspace of the original $H\_0^1$.

Typically, one has an algorithm for subdividing a given mesh. If the primary method for increasing precision is to subdivide the mesh, one has an h-method ( h is customarily the diameter of the largest element in the mesh.) In this manner, if one shows that the error with a grid $h$ is bounded above by $Ch^p$, for some and $p\; >\; 0$, then one has an order p method. Under specific hypotheses (for instance, if the domain is convex), a piecewise polynomial of order $d$ method will have an error of order $p\; =\; d+1$.

If instead of making h smaller, one increases the degree of the polynomials used in the basis function, one has a p-method. If one combines these two refinement types, one obtains an hp-method (hp-FEM). In the hp-FEM, the polynomial degrees can vary from element to element. High-order methods with large uniform p are called spectral finite element methods (SFEM). These are not to be confused with .

For vector partial differential equations, the basis functions may take values in $\backslash mathbb\{R\}^n$.

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Various types of finite element methods

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AEM The Applied Element Method or AEM combines features of both FEM and Discrete element method or (DEM).

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A-FEM Yang and Lui introduced the Augmented-Finite Element Method, whose goal was to model the weak and strong discontinuities without needing extra DoFs, as PuM stated.

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CutFEM The Cut Finite Element Approach was developed in 2014. The approach is "to make the discretization as independent as possible of the geometric description and minimize the complexity of mesh generation, while retaining the accuracy and robustness of a standard finite element method."

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Generalized finite element method The generalized finite element method (GFEM) uses local spaces consisting of functions, not necessarily polynomials, that reflect the available information on the unknown solution and thus ensure good local approximation. Then a partition of unity is used to “bond” these spaces together to form the approximating subspace. The effectiveness of GFEM has been shown when applied to problems with domains having complicated boundaries, problems with micro-scales, and problems with boundary layers.

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Mixed finite element method The mixed finite element method is a type of finite element method in which extra independent variables are introduced as nodal variables during the discretization of a partial differential equation problem.

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Variable – polynomial The hp-FEM combines adaptively elements with variable size h and polynomial degree p to achieve exceptionally fast, exponential convergence rates.P. Solin, K. Segeth, I. Dolezel: Higher-Order Finite Element Methods, Chapman & Hall/CRC Press, 2003

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hpk-FEM The hpk-FEM combines adaptively elements with variable size h, polynomial degree of the local approximations p, and global differentiability of the local approximations ( k-1) to achieve the best convergence rates.

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XFEM The extended finite element method (XFEM) is a numerical technique based on the generalized finite element method (GFEM) and the partition of unity method (PUM). It extends the classical finite element method by enriching the solution space for solutions to differential equations with discontinuous functions. Extended finite element methods enrich the approximation space to naturally reproduce the challenging feature associated with the problem of interest: the discontinuity, singularity, boundary layer, etc. It was shown that for some problems, such an embedding of the problem's feature into the approximation space can significantly improve convergence rates and accuracy. Moreover, treating problems with discontinuities with XFEMs suppresses the need to mesh and re-mesh the discontinuity surfaces, thus alleviating the computational costs and projection errors associated with conventional finite element methods at the cost of restricting the discontinuities to mesh edges.

Several research codes implement this technique to various degrees:

1. GetFEM++
2. xfem++
3. openxfem++

XFEM has also been implemented in codes like Altair Radios, ASTER, Morfeo, and Abaqus. It is increasingly being adopted by other commercial finite element software, with a few plugins and actual core implementations available (ANSYS, SAMCEF, OOFELIE, etc.).

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Scaled boundary finite element method (SBFEM) The introduction of the scaled boundary finite element method (SBFEM) came from Song and Wolf (1997). The SBFEM has been one of the most profitable contributions in the area of numerical analysis of fracture mechanics problems. It is a semi-analytical fundamental-solutionless method combining the advantages of finite element formulations and procedures and boundary element discretization. However, unlike the boundary element method, no fundamental differential solution is required.

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S-FEM The S-FEM, Smoothed Finite Element Methods, is a particular class of numerical simulation algorithms for the simulation of physical phenomena. It was developed by combining mesh-free methods with the finite element method.

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Spectral element method Spectral element methods combine the geometric flexibility of finite elements and the acute accuracy of spectral methods. Spectral methods are the approximate solution of weak-form partial equations based on high-order Lagrangian interpolants and used only with certain quadrature rules.

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Meshfree methods

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Discontinuous Galerkin methods

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Finite element limit analysis

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Stretched grid method

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Loubignac iteration Loubignac iteration is an iterative method in finite element methods.

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Crystal plasticity finite element method (CPFEM) The crystal plasticity finite element method (CPFEM) is an advanced numerical tool developed by Franz Roters. Metals can be regarded as crystal aggregates, which behave anisotropy under deformation, such as abnormal stress and strain localization. CPFEM, based on the slip (shear strain rate), can calculate dislocation, crystal orientation, and other texture information to consider crystal anisotropy during the routine. It has been applied in the numerical study of material deformation, surface roughness, fractures, etc.

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Virtual element method (VEM) The virtual element method (VEM), introduced by Beirão da Veiga et al. (2013) as an extension of mimetic finite difference (MFD) methods, is a generalization of the standard finite element method for arbitrary element geometries. This allows admission of general polygons (or polyhedra in 3D) that are highly irregular and non-convex in shape. The name virtual derives from the fact that knowledge of the local shape function basis is not required and is, in fact, never explicitly calculated.

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Link with the gradient discretization method Some types of finite element methods (conforming, nonconforming, mixed finite element methods) are particular cases of the gradient discretization method (GDM). Hence the convergence properties of the GDM, which are established for a series of problems (linear and nonlinear elliptic problems, linear, nonlinear, and degenerate parabolic problems), hold as well for these particular FEMs.

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Comparison to the finite difference method The finite difference method (FDM) is an alternative way of approximating solutions of PDEs. The differences between FEM and FDM are:

• The most attractive feature of the FEM is its ability to handle complicated geometries (and boundaries) with relative ease. While FDM in its basic form is restricted to handle rectangular shapes and simple alterations thereof, the handling of geometries in FEM is theoretically straightforward.
• FDM is not usually used for irregular CAD geometries but more often for rectangular or block-shaped models.
• FEM generally allows for more flexible mesh adaptivity than FDM.
• The most attractive feature of finite differences is that it is straightforward to implement.
• One could consider the FDM a particular case of the FEM approach in several ways. E.g., first-order FEM is identical to FDM for Poisson's equation if the problem is Discretization by a regular rectangular mesh with each rectangle divided into two triangles.
• There are reasons to consider the mathematical foundation of the finite element approximation more sound, for instance, because the quality of the approximation between grid points is poor in FDM.
• The quality of a FEM approximation is often higher than in the corresponding FDM approach, but this is highly problem-dependent, and several examples to the contrary can be provided.

Generally, FEM is the method of choice in all types of analysis in structural mechanics (i.e., solving for deformation and stresses in solid bodies or dynamics of structures). In contrast, computational fluid dynamics (CFD) tend to use FDM or other methods like finite volume method (FVM). CFD problems usually require discretization of the problem into a large number of cells/gridpoints (millions and more). Therefore the cost of the solution favors simpler, lower-order approximation within each cell. This is especially true for 'external flow' problems, like airflow around the car, airplane, or weather simulation.

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Finite element and fast fourier transform (FFT) methods Another method used for approximating solutions to a partial differential equation is the Fast Fourier Transform (FFT), where the solution is approximated by a fourier series computed using the FFT. For approximating the mechanical response of materials under stress, FFT is often much faster, but FEM may be more accurate. One example of the respective advantages of the two methods is in simulation of rolling a sheet of Aluminium (an FCC metal), and Wire drawing a wire of tungsten (a BCC metal). This simulation did not have a sophisticated shape update algorithm for the FFT method. In both cases, the FFT method was more than 10 times as fast as FEM, but in the wire drawing simulation, where there were large deformations in Crystallite, the FEM method was much more accurate. In the sheet rolling simulation, the results of the two methods were similar. FFT has a larger speed advantage in cases where the boundary conditions are given in the materials strain, and loses some of its efficiency in cases where the stress is used to apply the boundary conditions, as more iterations of the method are needed.

The FE and FFT methods can also be combined in a voxel based method (2) to simulate deformation in materials, where the FE method is used for the macroscale stress and deformation, and the FFT method is used on the microscale to deal with the effects of microscale on the mechanical response. Unlike FEM, FFT methods’ similarities to image processing methods means that an actual image of the microstructure from a microscope can be input to the solver to get a more accurate stress response. Using a real image with FFT avoids meshing the microstructure, which would be required if using FEM simulation of the microstructure, and might be difficult. Because fourier approximations are inherently periodic, FFT can only be used in cases of periodic microstructure, but this is common in real materials. FFT can also be combined with FEM methods by using fourier components as the variational basis for approximating the fields inside an element, which can take advantage of the speed of FFT based solvers.

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Application

Various specializations under the umbrella of the mechanical engineering discipline (such as aeronautical, biomechanical, and automotive industries) commonly use integrated FEM in the design and development of their products. Several modern FEM packages include specific components such as thermal, electromagnetic, fluid, and structural working environments. In a structural simulation, FEM helps tremendously in producing stiffness and strength visualizations and minimizing weight, materials, and costs.

This powerful design tool has significantly improved both the standard of engineering designs and the design process methodology in many industrial applications.Hastings, J. K., Juds, M. A., Brauer, J. R., Accuracy and Economy of Finite Element Magnetic Analysis, 33rd Annual National Relay Conference, April 1985. The introduction of FEM has substantially decreased the time to take products from concept to the production line. Testing and development have been accelerated primarily through improved initial prototype designs using FEM. In summary, benefits of FEM include increased accuracy, enhanced design and better insight into critical design parameters, virtual prototyping, fewer hardware prototypes, a faster and less expensive design cycle, increased productivity, and increased revenue.

In the 1990s FEM was proposed for use in stochastic modeling for numerically solving probability models and later for reliability assessment.

(2025). 9780471369615, John Wiley & Sons. ISBN 9780471369615

FEM is widely applied for approximating differential equations that describe physical systems. This method is very popular in the community of Computational fluid dynamics, and there are many applications for solving Navier–Stokes equations with FEM.

(1986). 9781402003097, Springer Science & Business Media. ISBN 9781402003097

(2025). 9783642648885, Springer Science & Business Media. ISBN 9783642648885

Recently, the application of FEM has been increasing in the researches of computational plasma. Promising numerical results using FEM for Magnetohydrodynamics, Vlasov equation, and Schrödinger equation have been proposed.

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See also

• Applied element method
• Boundary element method
• Céa's lemma
• Computer experiment
• Direct stiffness method
• Discontinuity layout optimization
• Discrete element method
• Finite difference method
• Finite element machine
• Finite element method in structural mechanics
• Finite volume method
• Finite volume method for unsteady flow
• Infinite element method
• Interval finite element
• Isogeometric analysis
• Lattice Boltzmann methods
• List of finite element software packages
• Meshfree methods
• Movable cellular automaton
• Multidisciplinary design optimization
• Multiphysics
• Patch test
• Rayleigh–Ritz method
• SDC Verifier
• Space mapping
• STRAND7
• Tessellation (computer graphics)
• Weakened weak form

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Further reading

• G. Allaire and A. Craig: Numerical Analysis and Optimization: An Introduction to Mathematical Modelling and Numerical Simulation.
• K. J. Bathe: Numerical methods in finite element analysis, Prentice-Hall (1976).
• Thomas J.R. Hughes: The Finite Element Method: Linear Static and Dynamic Finite Element Analysis, Prentice-Hall (1987).
• J. Chaskalovic: Finite Elements Methods for Engineering Sciences, Springer Verlag, (2008).
• Endre Süli: Finite Element Methods for Partial Differential Equations.
• O. C. Zienkiewicz, R. L. Taylor, J. Z. Zhu : The Finite Element Method: Its Basis and Fundamentals, Butterworth-Heinemann (2005).
• N. Ottosen, H. Petersson: Introduction to the Finite Element Method, Prentice-Hall (1992).
• Susanne C. Brenner, L. Ridgway Scott: The Mathematical Theory of Finite Element Methods, Springer-Verlag New York, ISBN 978-0-387-75933-3 (2008).
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• Leszek F. Demkowicz: Mathematical Theory of Finite Elements, SIAM, ISBN 978-1-61197-772-1 (2024).

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