Isogeometric mortaring
|
|
- Martin Paul
- 5 years ago
- Views:
Transcription
1 Isogeometric mortaring E. Brivadis, A. Buffa, B. Wohlmuth, L. Wunderlich IMATI E. Magenes - Pavia Technical University of Munich A. Buffa (IMATI-CNR Italy) IGA mortaring 1 / 29
2 1 Introduction Splines Approximation spaces and properties 2 Non conforming interfaces Mortar method Numerical validation 3 Final remarks A. Buffa (IMATI-CNR Italy) IGA mortaring 2 / 29
3 IGA is based on spline theory B-Splines are defined by the Cox-DeBoor formulae: { 1 if ξi ζ < ξ N i,0 (ζ) = i+1, 0 otherwise, N i,p (ζ) = ζ ξ i N i,p 1 (ζ) + ξ i+p+1 ζ N i+1,p 1 (ζ). ξ i+p ξ i ξ i+p+1 ξ i+1 A. Buffa (IMATI-CNR Italy) IGA mortaring 3 / 29
4 ξ" Quadratic (p=2) basis functions for an non-uniform based onopen, spline theory knot vector:5! 4 IGA is B-Splines are defined by the formulae:" Ξ =Cox-DeBoor {0,0,0,1,2,3,4,4,5,5,5} 1 if ξi ζ < ξi+1, Ni,0 (ζ) = 0 ξ" 0 otherwise, ξ" ξi+p+1 ζ ζ ξi 1 Ni,p (ζ) = Ni,p 1 (ζ) + Ni+1,p 1 (ζ). ξi+p ξi - control pointsξi+p+1 ξi+1 - knots ts F(ξ) = P i Ci Ni,p (ξ) : Quadratic basis h-refined Curve control points A. Buffa (IMATI-CNR Italy) IGA mortaring knots 3 / 29
5 4 4 IGA is based on spline theory B-Splines are defined by the Cox-DeBoor formulae: 6/18/ if ξi ζ < ξi+1, 2 Ni,0 (ζ) = 0 0 otherwise, h-refined Surface ξi+p+1 ζ ζ ξi 1 Ni,p (ζ) = Ni,p 1 (ζ) + Ni+1,p 1 (ζ). ξi+p ξi - control pointsξi+p+1 ξi+1 - knots ts F(ξ) = P i Ci Ni,p (ξ) : Quadratic basis h-refined Surface Control net Mesh Control net A. Buffa (IMATI-CNR Italy) IGA mortaring 3 / 29
6 4 4 IGA is based on spline theory B-Splines are defined by the Cox-DeBoor formulae: 6/18/ if ξi ζ < ξi+1, 2 Ni,0 (ζ) = 0 0 otherwise, h-refined Surface ξi+p+1 ζ ζ ξi 1 Ni,p (ζ) = Ni,p 1 (ζ) + Ni+1,p 1 (ζ). ξi+p ξi - control pointsξi+p+1 ξi+1 - knots ts F(ξ) = P i Ci Ni,p (ξ) : Quadratic basis h-refined Surface Control net NURBS: projection of splines in Rd+1... no need for thismesh talk. Control net A. Buffa (IMATI-CNR Italy) IGA mortaring 3 / 29
7 Construction of approximation spaces F The geometry Ω and its NURBS parametrization F is given by CAD general geometry: unstructured collection of patches. A. Buffa (IMATI-CNR Italy) IGA mortaring 4 / 29
8 Construction of approximation spaces F The geometry Ω and its NURBS parametrization F is given by CAD general geometry: unstructured collection of patches. The discrete space on Ω is the push-forward of Spline/NURBS A. Buffa (IMATI-CNR Italy) IGA mortaring 4 / 29
9 Construction of approximation spaces F The geometry Ω and its NURBS parametrization F is given by CAD general geometry: unstructured collection of patches. The discrete space on Ω is the push-forward of Spline/NURBS Refinement by knot insertion and degree elevation, geometry unchanged. A. Buffa (IMATI-CNR Italy) IGA mortaring 4 / 29
10 Construction of approximation spaces F The geometry Ω and its NURBS parametrization F is given by CAD general geometry: unstructured collection of patches. The discrete space on Ω is the push-forward of Spline/NURBS Refinement by knot insertion and degree elevation, geometry unchanged. A. Buffa (IMATI-CNR Italy) IGA mortaring 4 / 29
11 General geometries are multi-patch Ω (2) Ω (1) Ω (3) (b) T-shaped, but not hanging Globally unstructured Locally structured A. Buffa (IMATI-CNR Italy) IGA mortaring 5 / 29
12 General geometries are multi-patch Ω (2) Ω (1) Ω (3) (b) T-shaped, but not hanging Globally unstructured Locally structured A. Buffa (IMATI-CNR Italy) IGA mortaring 5 / 29
13 General geometries are multi-patch Ω (2) Ω (1) Ω (3) (b) T-shaped, but not hanging Globally unstructured Locally structured Question: How to enhance flexibility? Question: How to treat non conforming interfaces? A. Buffa (IMATI-CNR Italy) IGA mortaring 5 / 29
14 Perfect setting for adaptivity if splines can support local refinement T-splines : Pure geometric modeling approach: Sederberg et al 2004, Hughes, Scott, Evans, Li, Zhang,... Pavia team courtesy of M. Scott LR-splines Dokken et al. 2013, Bressan 2013 Definition R n, spline theory of LR-Splines Hierarchical splines Kraft 1998,... the closest to adaptive finite elements on quadrangular meshes A. Buffa (IMATI-CNR Italy) IGA mortaring 6 / 29
15 Hierarchical splines Kraft 1998, Giannelli, Jüttler, Simeon, Speelers, Voung , B.-Giannelli C. Giannelli et al. / Computer Aided Geometric Design 29 (2012) ins (b) hierarchical mesh (a) nested domains (b) hierarchical me Fig. thesplinehierarchyaccordingtorelation(1),i.e.,ω l 2. Anestedsequenceofdomainsfortheconstructionofthesplinehierarchyaccordingtorelation(1),i.e.,Ω Ω l+1 for l = 0,...,2, for the two- l dimensional case. (a) Only dyadic refinement is considered. (b) Ω l+1 is restricted to be the union of supports of B-splines of level l. (c) The boundaries of adjacent domains Ω s of B-splines of level l. l and Ω l+1 must be disjoint. Ω l+1 (d) The modified support definition (2) is not used and H 0 is initialized as the set of B-s must be disjoint. ed and H 0 completely contained is initialized as the set of B-splines in B 0 in Ω 0. whose support is Moreover, the definition in Kraft s thesis (Kraft, 1998) additionally considers the auxiliary su ω l = { x Ω l β B l : x supp β supp β Ω l }, 98) additionally considers the auxiliary subdomain for l = 0,...,N 1, which represents the biggest subset of Ω l such that H l B spans the restr that these subdomains are nested as well, A. Buffa (IMATI-CNR Italy) IGA mortaring 7 / 29 p β Ω l},
16 Hierarchical splines Kraft 1998, Giannelli, Jüttler, Simeon, Speelers, Voung , B.-Giannelli C. Giannelli et al. / Computer Aided Geometric Design 29 (2012) ins (b) hierarchical mesh (a) nested domains (b) hierarchical me Fig. thesplinehierarchyaccordingtorelation(1),i.e.,ω l 2. Anestedsequenceofdomainsfortheconstructionofthesplinehierarchyaccordingtorelation(1),i.e.,Ω Ω l+1 for l = 0,...,2, for the two- l dimensional case. (a) Only dyadic refinement is considered. (b) Ω l+1 is restricted to be the union of supports of B-splines of level l. (c) The boundaries of adjacent domains Ω s of B-splines of level l. l and Ω l+1 must be disjoint. Definition of truncated-basis Ω l+1 (d) The modified ensuring support definition good (2) isspline not used and properties H 0 is initialized as the set of B-s must be disjoint. ed and H 0 completely contained is initialized as the set of B-splines in B 0 in Ω 0. whose support is Giannelli, Juettler, Speelers Moreover, the definition in Kraft s thesis (Kraft, 1998) additionally considers the auxiliary su ω l = { x Ω l β B l : x supp β supp β Ω l }, 98) additionally considers the auxiliary subdomain for l = 0,...,N 1, which represents the biggest subset of Ω l such that H l B spans the restr that these subdomains are nested as well, A. Buffa (IMATI-CNR Italy) IGA mortaring 7 / 29 p β Ω l}, V 0 V 1 V 2... V J Refinement has to contain at least one function : (p + 1) 2 elements
17 Adaptivity with hierarchical splines B. and Giannelli, 2014 Residual based estimator: η Q = h Q Au h f L 2 (Q) (no jumps) Dörfler marking E(u h, M) θe(u h, T), 0 < θ < 1; Suitable local quasi-interpolant and their approximation properties A. Buffa (IMATI-CNR Italy) IGA mortaring 8 / 29
18 Adaptivity with hierarchical splines B. and Giannelli, 2014 Residual based estimator: η Q = h Q Au h f L 2 (Q) (no jumps) Dörfler marking E(u h, M) θe(u h, T), 0 < θ < 1; Suitable local quasi-interpolant and their approximation properties The theory of adaptive methods Convergence and optimality! Morin, Nochetto, Siebert Binev, Dahmen, DeVore A. Buffa (IMATI-CNR Italy) IGA mortaring 8 / 29
19 Adaptivity with hierarchical splines B. and Giannelli, 2014 Residual based estimator: η Q = h Q Au h f L 2 (Q) (no jumps) Dörfler marking E(u h, M) θe(u h, T), 0 < θ < 1; Suitable local quasi-interpolant and their approximation properties The theory of adaptive methods Convergence and optimality!... but this is another story... Morin, Nochetto, Siebert Binev, Dahmen, DeVore A. Buffa (IMATI-CNR Italy) IGA mortaring 8 / 29
20 Non conforming interfaces and mortaring A. Buffa (IMATI-CNR Italy) IGA mortaring 9 / 29
21 Non conforming interfaces and mortaring Let Ω be a computational domain in R n, we want to solve the Laplace problem (or linear elasticity with minor changes) div (A u) = f with boundary conditions Ω = Γ D Γ N. u = 0 on Γ D and (A u) n = h on Γ N We suppose that Ω = N i Ω i, Ω i = F i ( Ω), Γ ij = Ω i Ω j, F i are splines (or NURBS) non compatible meshes at the interfaces Γ ij A. Buffa (IMATI-CNR Italy) IGA mortaring 9 / 29
22 About the admissible partition of the domain m(2) 1 s(1) n 2 n 1 s(2) m(1) s(1) n 1 2 s(2) n 2 m(1) m(2) 3 Decomposition can be conforming or non-conforming We can handle the case when Γ ij is a face of either Ω i or Ω j. There is the need for cross-point treatment/reduction A. Buffa (IMATI-CNR Italy) IGA mortaring 10 / 29
23 About the admissible partition of the domain m(2) 1 s(1) n 2 n 1 s(2) m(1) s(1) n 1 2 s(2) n 2 m(1) m(2) 3 Decomposition can be conforming or non-conforming We can handle the case when Γ ij is a face of either Ω i or Ω j. There is the need for cross-point treatment/reduction Non compatible geometries interfaces at the interfaces Γ ij (?) A. Buffa (IMATI-CNR Italy) IGA mortaring 10 / 29
24 Non conforming interfaces and mortaring Let S p ( T j ) be the space of tensor product splines/nurbs of degree p, on the knot mesh T j. in each subdomain Ω j, V j = {v j H 1 (Ω j ) : v F j S p ( T j )} A. Buffa (IMATI-CNR Italy) IGA mortaring 11 / 29
25 Non conforming interfaces and mortaring Let S p ( T j ) be the space of tensor product splines/nurbs of degree p, on the knot mesh T j. in each subdomain Ω j, V j = {v j H 1 (Ω j ) : v F j S p ( T j )} N V = {v L 2 (Ω) : v Ωj V j, v ΓD = 0} v 2 V = v 2 H 1 (Ω j ). i=1 A. Buffa (IMATI-CNR Italy) IGA mortaring 11 / 29
26 Non conforming interfaces and mortaring Let S p ( T j ) be the space of tensor product splines/nurbs of degree p, on the knot mesh T j. in each subdomain Ω j, V j = {v j H 1 (Ω j ) : v F j S p ( T j )} N V = {v L 2 (Ω) : v Ωj V j, v ΓD = 0} v 2 V = v 2 H 1 (Ω j ). Interface numbering and spaces Σ 0 = n I l=1 i=1 Γ l, l (i l, j l ) : Γ l = Ω il Ω jl. Continuity across Σ 0 imposed via Lagrange multipliers: M = {λ L 2 (Σ 0 ) : λ l = λ Γl M l } M l to be chosen properly! A. Buffa (IMATI-CNR Italy) IGA mortaring 11 / 29
27 Variational formulation of the problem Find u h V, λ h M such that a(u h, v h )+b(λ h, v h ) = R(v h ) b(µ h, u h ) = 0 v h V µ h M where a(u, v) = A u v b(λ, v) = λ l [u] [u] = u il u jl Ω l Γ l R(v) is the RHS taking into account also Neumann BC... A. Buffa (IMATI-CNR Italy) IGA mortaring 12 / 29
28 Variational formulation of the problem Find u h V, λ h M such that a(u h, v h )+b(λ h, v h ) = R(v h ) b(µ h, u h ) = 0 v h V µ h M where a(u, v) = A u v b(λ, v) = λ l [u] [u] = u il u jl Ω l Γ l R(v) is the RHS taking into account also Neumann BC... Wellposedness and approximation depends only upon the choice of Lagrange multipliers which should guarantee stability! A. Buffa (IMATI-CNR Italy) IGA mortaring 12 / 29
29 Variational formulation of the problem Find u h V, λ h M such that a(u h, v h )+b(λ h, v h ) = R(v h ) b(µ h, u h ) = 0 v h V µ h M where a(u, v) = A u v b(λ, v) = λ l [u] [u] = u il u jl Ω l Γ l R(v) is the RHS taking into account also Neumann BC... Wellposedness and approximation depends only upon the choice of Lagrange multipliers which should guarantee stability! M = {λ L 2 (Σ 0 ) : λ l = λ Γl M l } n I λ 2 M = λ l 2 (H 1/2 00 ) l=1 A. Buffa (IMATI-CNR Italy) IGA mortaring 12 / 29
30 Choice of the Langrange multiplier space Topology for M l is H 1/2 00 (Γ l) I want to have the largest possible set of multipliers such that the form b(λ, v) = Γ l λ l [u] remains uniformly stable Favorite choice: if i l is the slave side, we want M l V il Γl! It contraints all slave functions. But it is known that stability fails with this choice, and there is a need for cross point degree reduction.. A. Buffa (IMATI-CNR Italy) IGA mortaring 13 / 29
31 Choice of the Langrange multiplier space Topology for M l is H 1/2 00 (Γ l) I want to have the largest possible set of multipliers such that the form b(λ, v) = Γ l λ l [u] remains uniformly stable Favorite choice: if i l is the slave side, we want M l V il Γl! It contraints all slave functions. But it is known that stability fails with this choice, and there is a need for cross point degree reduction.. dim(m l ) dim{v V il Γl : v Γl = 0} A. Buffa (IMATI-CNR Italy) IGA mortaring 13 / 29
32 Choice of the Langrange multiplier space Each Γ l is a face of a subdomain Ω i (the slave side) Γ l inherits a spline mapping F l : (0, 1) d 1 Γ l and a parametric mesh on Γ = (0, 1) d 1 denoted as T l. A. Buffa (IMATI-CNR Italy) IGA mortaring 14 / 29
33 Choice of the Langrange multiplier space Each Γ l is a face of a subdomain Ω i (the slave side) Γ l inherits a spline mapping F l : (0, 1) d 1 Γ l and a parametric mesh on Γ = (0, 1) d 1 denoted as T l. Let us start with choices in the parametric space, and then we will map! A. Buffa (IMATI-CNR Italy) IGA mortaring 14 / 29
34 Choice of the Langrange multiplier space Each Γ l is a face of a subdomain Ω i (the slave side) Γ l inherits a spline mapping F l : (0, 1) d 1 Γ l and a parametric mesh on Γ = (0, 1) d 1 denoted as T l. Let us start with choices in the parametric space, and then we will map! Choice 1: same degree, cross point reduction M l 1 = S p ( T l ) 2 1 i h 2h 3h ζ A. Buffa (IMATI-CNR Italy) IGA mortaring 14 / 29
35 Choice of the Langrange multiplier space Each Γ l is a face of a subdomain Ω i (the slave side) Γ l inherits a spline mapping F l : (0, 1) d 1 Γ l and a parametric mesh on Γ = (0, 1) d 1 denoted as T l. Let us start with choices in the parametric space, and then we will map! Choice 2: degree reduction M l 2 = S p 2( T l ) Indeed, it is true that dim( M l 2 ) = { v S p( T il ) Γl : v Γl = 0} No need for degree reduction or other manipulation If stable, it will deliver a slightly suboptimal order : 1/2 suboptimal A. Buffa (IMATI-CNR Italy) IGA mortaring 14 / 29
36 Stability: numerical checks Chapelle-Bathe test Estimate on the inf-sup constant: A. Buffa (IMATI-CNR Italy) IGA mortaring 15 / 29
37 Stability: numerical checks Chapelle-Bathe test Estimate on the inf-sup constant: Testing M l against S p ( T il ) Γl without boundary conditions Stability constant Inverse of the number of elements P5 P5 P5 P4 P5 P3 P5 P2 P5 P1 P5 P0 O(E 1 ) Stability constant Pp Pp Pp P(p 2) Pp P(p 4) p p/p 2k couples are all stable! the pairings are also stable varying p! A. Buffa (IMATI-CNR Italy) IGA mortaring 15 / 29
38 Stability: numerical checks Chapelle-Bathe test Estimate on the inf-sup constant: Testing M l against S p ( T il ) Γl with boundary conditions... the right thing! 1 Stability constant P5 P5 P5 P3 P5 P Inverse of the number of elements Stability constant Pp Pp Pp P(p 2) Pp P(p 4) p p/p 2k couples are all stable! exponential behavior in p! A. Buffa (IMATI-CNR Italy) IGA mortaring 15 / 29
39 Stability: Proof of the inf-sup condition the p/p 2 case We consider M l 2 and can prove the following: µ v Γ inf sup α 0 v L 2 µ L 2 + quasi uniform meshes : inf µ S p 2 v S p H0 1 sup µ S p 2 v S p H0 1 µ v Γ α 0 v 1/2 H µ 1/2 00 (H 00 ) A. Buffa (IMATI-CNR Italy) IGA mortaring 16 / 29
40 Stability: Proof of the inf-sup condition the p/p 2 case We consider M l 2 and can prove the following: µ v Γ inf sup α 0 v L 2 µ L 2 + quasi uniform meshes : Proof In 2D: S p H0 1 x inf µ S p 2 v S p H0 1 sup µ S p 2 v S p H0 1 x µ v Γ α 0 v 1/2 H µ 1/2 00 (H 00 ) Sp 1 L 2 0 Sp 2 is exact choose v S p H0 1 such that 2 xx v = µ and the work with Sobolev norms. In 3D, basically the same applies... A. Buffa (IMATI-CNR Italy) IGA mortaring 16 / 29
41 Stability: Proof of the inf-sup condition the p/p 2 case We consider M l 2 and can prove the following: µ v Γ inf sup α 0 v L 2 µ L 2 + quasi uniform meshes : Proof In 2D: S p H0 1 x inf µ S p 2 v S p H0 1 sup µ S p 2 v S p H0 1 x µ v Γ α 0 v 1/2 H µ 1/2 00 (H 00 ) Sp 1 L 2 0 Sp 2 is exact choose v S p H0 1 such that 2 xx v = µ and the work with Sobolev norms. In 3D, basically the same applies... It is stable!... we need now to go to physical space A. Buffa (IMATI-CNR Italy) IGA mortaring 16 / 29
42 Stability in the physical space the p/p 2 case inf sup µ S p 2 v S p H0 1 Γ µ v v L 2 µ L 2 α 0 inf sup µ M l v V il :v H0 1(Γ l) Γ l µ v v L 2 µ L 2 α 0 A. Buffa (IMATI-CNR Italy) IGA mortaring 17 / 29
43 Stability in the physical space the p/p 2 case inf sup µ S p 2 v S p H0 1 Γ µ v v L 2 µ L 2 α 0 inf sup µ M l v V il :v H0 1(Γ l) Γ l µ v v L 2 µ L 2 α 0 Γ l µ v = Γ ρ µ v ρ = weight, area change.. A. Buffa (IMATI-CNR Italy) IGA mortaring 17 / 29
44 Stability in the physical space the p/p 2 case inf sup µ S p 2 v S p H0 1 Γ µ v v L 2 µ L 2 α 0 inf sup µ M l v V il :v H0 1(Γ l) Γ l µ v v L 2 µ L 2 Γ l µ v = Γ ρ µ v ρ = weight, area change.. and by super-convergence results à la Wahlbin: α 0 Π : L 2 ( Γ) M 2 l ρ µ Π(ρ µ) L 2 ( Γ) Ch µ L 2 ( Γ) A. Buffa (IMATI-CNR Italy) IGA mortaring 17 / 29
45 Stability in the physical space the p/p 2 case inf sup µ S p 2 v S p H0 1 Γ µ v v L 2 µ L 2 α 0 inf sup µ M l v V il :v H0 1(Γ l) Γ l µ v v L 2 µ L 2 Γ l µ v = Γ ρ µ v ρ = weight, area change.. and by super-convergence results à la Wahlbin: α 0 Π : L 2 ( Γ) M 2 l ρ µ Π(ρ µ) L 2 ( Γ) Ch µ L 2 ( Γ) For h small enough the stability holds in physical space! A. Buffa (IMATI-CNR Italy) IGA mortaring 17 / 29
46 Back to our variational problem Find u h V, λ h M such that a(u h, v h )+b(λ h, v) = R(v h ) b(µ h, u h ) = 0 v h V µ h M A. Buffa (IMATI-CNR Italy) IGA mortaring 18 / 29
47 Back to our variational problem Find u h V, λ h M such that a(u h, v h )+b(λ h, v) = R(v h ) b(µ h, u h ) = 0 v h V µ h M It is well-posed and verifies the following error estimate: if u H r (Ω): u u h V C inf v h V u v h V + inf µ h M λ µ h M (1) Ch t + Ch s t = min{p, r 1} (2) s = min{p + 1/2, r 1} for Choice 1: same degree, s = min{p 1/2, r 1} for Choice 2: degree reduction Or, indeed: u u h V C inf u v h V C... v h V Ker(B) A. Buffa (IMATI-CNR Italy) IGA mortaring 18 / 29
48 Numerical validation: problem Ω 1 γ γ 3 γ 2 Ω 3 1 Ω A. Buffa (IMATI-CNR Italy) IGA mortaring 19 / 29
49 Numerical validation: problem u uh V Mortar P4 P4 Mortar P4 P2 Mortar P3 P3 Mortar P3 P1 O(h 2/3 ) u n λ h L 2 (γ 2) Mortar P4 P4 Mortar P4 P2 Mortar P3 P3 Mortar P3 P1 O(h 1/6 ) primal dof number primal dof number 1/6 + 1/2 = 2/3 A. Buffa (IMATI-CNR Italy) IGA mortaring 20 / 29
50 Numerical validation: problem A. Buffa (IMATI-CNR Italy) IGA mortaring 21 / 29
51 Numerical validation: problem 2 u uh L 2 (Ω ) Mortar P4 P4 Mortar P4 P2 Conform P4 O(h 5 ) u uh L 2 (Ω ) Mortar P3 P3 Mortar P3 P1 Conform P3 O(h 4 ) primal dof number primal dof number Multipliers degree does not affect the order for the primal unknown! A. Buffa (IMATI-CNR Italy) IGA mortaring 22 / 29
52 Numerical validation: problem u n λ h L 2 (Γ) Mortar P4 P4 Mortar P4 P2 Mortar P3 P3 Mortar P3 P1 O(h 2 ), O(h 3 ), O(h 4 ),O(h 5 ) primal dof number but it affects the convergence of the multiplier! A. Buffa (IMATI-CNR Italy) IGA mortaring 23 / 29
53 Numerical validation: elasticity A. Buffa (IMATI-CNR Italy) IGA mortaring 24 / 29
54 Numerical validation: elasticity u uh V Mortar P4 P4 Mortar P4 P2 Mortar P4 P0 O(h 2 ), O(h 4 ) u uh V Mortar P4 P4 Mortar P4 P2 Mortar P4 P0 O(h 2 ), O(h 4 ) primal dof number primal dof number A. Buffa (IMATI-CNR Italy) IGA mortaring 25 / 29
55 Numerical validation: elasticity σ n λ h L 2 (Γ ) Mortar P4 P4 Mortar P4 P2 Mortar P4 P0 O(h), O(h 3 ), O(h 4 ) σ n λ h L 2 (Γ ) Mortar P4 P4 Mortar P4 P2 Mortar P4 P0 O(h), O(h 3 ), O(h 4 ) primal dof number primal dof number A. Buffa (IMATI-CNR Italy) IGA mortaring 26 / 29
56 Final remarks This approach can be used to treat contact in a variationally consistent way For patch gluing: the geometric non-matching patch cases should be studied in details The question of exact / inexact integration for interface integrals remains open (robustness of splines thanks to regularity) A. Buffa (IMATI-CNR Italy) IGA mortaring 27 / 29
57 Final remarks Surveys and Codes New Acta Numerica survey paper with several math results: L. Beirão Da Veiga, A. Buffa, G. Sangalli, R. Vázquez, Mathematical analysis of variational isogeometric methods We have two codes available to public : GeoPDEs library is a GNU licensed software available here: IGATools is a C++ dimension independent library igatools A. Buffa (IMATI-CNR Italy) IGA mortaring 28 / 29
58 THANKS! A. Buffa (IMATI-CNR Italy) IGA mortaring 29 / 29
PhD dissertation defense
Isogeometric mortar methods with applications in contact mechanics PhD dissertation defense Brivadis Ericka Supervisor: Annalisa Buffa Doctor of Philosophy in Computational Mechanics and Advanced Materials,
More informationAn introduction to Isogeometric Analysis
An introduction to Isogeometric Analysis A. Buffa 1, G. Sangalli 1,2, R. Vázquez 1 1 Istituto di Matematica Applicata e Tecnologie Informatiche - Pavia Consiglio Nazionale delle Ricerche 2 Dipartimento
More informationIsogeometric Analysis:
Isogeometric Analysis: some approximation estimates for NURBS L. Beirao da Veiga, A. Buffa, Judith Rivas, G. Sangalli Euskadi-Kyushu 2011 Workshop on Applied Mathematics BCAM, March t0th, 2011 Outline
More informationGeoPDEs. An Octave/Matlab software for research on IGA. R. Vázquez. IMATI Enrico Magenes, Pavia Consiglio Nazionale della Ricerca
GeoPDEs An Octave/Matlab software for research on IGA R. Vázquez IMATI Enrico Magenes, Pavia Consiglio Nazionale della Ricerca Joint work with C. de Falco and A. Reali Supported by the ERC Starting Grant:
More informationIsogeometric modeling of Lorentz detuning in linear particle accelerator cavities
Isogeometric modeling of Lorentz detuning in linear particle accelerator cavities Mauro Bonafini 1,2, Marcella Bonazzoli 3, Elena Gaburro 1,2, Chiara Venturini 1,3, instructor: Carlo de Falco 4 1 Department
More informationDual-Primal Isogeometric Tearing and Interconnecting Solvers for Continuous and Discontinuous Galerkin IgA Equations
Dual-Primal Isogeometric Tearing and Interconnecting Solvers for Continuous and Discontinuous Galerkin IgA Equations Christoph Hofer and Ulrich Langer Doctoral Program Computational Mathematics Numerical
More informationConvergence and optimality of an adaptive FEM for controlling L 2 errors
Convergence and optimality of an adaptive FEM for controlling L 2 errors Alan Demlow (University of Kentucky) joint work with Rob Stevenson (University of Amsterdam) Partially supported by NSF DMS-0713770.
More informationAdaptative isogeometric methods with hierarchical splines: optimality and convergence rates
MATHICSE Institute of Mathematics School of Basic Sciences MATHICSE Technical Report Nr. 08.2017 March 2017 Adaptative isogeometric methods with hierarchical splines: optimality and convergence rates Annalisa
More informationAdaptive Finite Element Methods Lecture 1: A Posteriori Error Estimation
Adaptive Finite Element Methods Lecture 1: A Posteriori Error Estimation Department of Mathematics and Institute for Physical Science and Technology University of Maryland, USA www.math.umd.edu/ rhn 7th
More informationThe space of C 1 -smooth isogeometric spline functions on trilinearly parameterized volumetric two-patch domains. Katharina Birner and Mario Kapl
The space of C 1 -smooth isogeometric spline functions on trilinearly parameterized volumetric two-patch domains Katharina Birner and Mario Kapl G+S Report No. 69 March 2018 The space of C 1 -smooth isogeometric
More informationFunctional type error control for stabilised space-time IgA approximations to parabolic problems
www.oeaw.ac.at Functional type error control for stabilised space-time IgA approximations to parabolic problems U. Langer, S. Matculevich, S. Repin RICAM-Report 2017-14 www.ricam.oeaw.ac.at Functional
More informationSpace-time Finite Element Methods for Parabolic Evolution Problems
Space-time Finite Element Methods for Parabolic Evolution Problems with Variable Coefficients Ulrich Langer, Martin Neumüller, Andreas Schafelner Johannes Kepler University, Linz Doctoral Program Computational
More informationIsogeometric Analysis with Geometrically Continuous Functions on Two-Patch Geometries
Isogeometric Analysis with Geometrically Continuous Functions on Two-Patch Geometries Mario Kapl a Vito Vitrih b Bert Jüttler a Katharina Birner a a Institute of Applied Geometry Johannes Kepler University
More informationINTRODUCTION TO FINITE ELEMENT METHODS
INTRODUCTION TO FINITE ELEMENT METHODS LONG CHEN Finite element methods are based on the variational formulation of partial differential equations which only need to compute the gradient of a function.
More informationMultipatch Space-Time Isogeometric Analysis of Parabolic Diffusion Problems. Ulrich Langer, Martin Neumüller, Ioannis Toulopoulos. G+S Report No.
Multipatch Space-Time Isogeometric Analysis of Parabolic Diffusion Problems Ulrich Langer, Martin Neumüller, Ioannis Toulopoulos G+S Report No. 56 May 017 Multipatch Space-Time Isogeometric Analysis of
More informationPARTITION OF UNITY FOR THE STOKES PROBLEM ON NONMATCHING GRIDS
PARTITION OF UNITY FOR THE STOES PROBLEM ON NONMATCHING GRIDS CONSTANTIN BACUTA AND JINCHAO XU Abstract. We consider the Stokes Problem on a plane polygonal domain Ω R 2. We propose a finite element method
More informationRemarks on the analysis of finite element methods on a Shishkin mesh: are Scott-Zhang interpolants applicable?
Remarks on the analysis of finite element methods on a Shishkin mesh: are Scott-Zhang interpolants applicable? Thomas Apel, Hans-G. Roos 22.7.2008 Abstract In the first part of the paper we discuss minimal
More informationAdaptive approximation of eigenproblems: multiple eigenvalues and clusters
Adaptive approximation of eigenproblems: multiple eigenvalues and clusters Francesca Gardini Dipartimento di Matematica F. Casorati, Università di Pavia http://www-dimat.unipv.it/gardini Banff, July 1-6,
More informationCondition number estimates for matrices arising in the isogeometric discretizations
www.oeaw.ac.at Condition number estimates for matrices arising in the isogeometric discretizations K. Gahalaut, S. Tomar RICAM-Report -3 www.ricam.oeaw.ac.at Condition number estimates for matrices arising
More informationImplementation of Sparse Wavelet-Galerkin FEM for Stochastic PDEs
Implementation of Sparse Wavelet-Galerkin FEM for Stochastic PDEs Roman Andreev ETH ZÜRICH / 29 JAN 29 TOC of the Talk Motivation & Set-Up Model Problem Stochastic Galerkin FEM Conclusions & Outlook Motivation
More informationELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS
ELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS CHARALAMBOS MAKRIDAKIS AND RICARDO H. NOCHETTO Abstract. It is known that the energy technique for a posteriori error analysis
More informationDomain Decomposition Preconditioners for Isogeometric Discretizations
Domain Decomposition Preconditioners for Isogeometric Discretizations Luca F Pavarino, Università di Milano, Italy Lorenzo Beirao da Veiga, Università di Milano, Italy Durkbin Cho, Dongguk University,
More informationAn optimal adaptive finite element method. Rob Stevenson Korteweg-de Vries Institute for Mathematics Faculty of Science University of Amsterdam
An optimal adaptive finite element method Rob Stevenson Korteweg-de Vries Institute for Mathematics Faculty of Science University of Amsterdam Contents model problem + (A)FEM newest vertex bisection convergence
More informationTwo-scale Dirichlet-Neumann preconditioners for boundary refinements
Two-scale Dirichlet-Neumann preconditioners for boundary refinements Patrice Hauret 1 and Patrick Le Tallec 2 1 Graduate Aeronautical Laboratories, MS 25-45, California Institute of Technology Pasadena,
More informationAdaptive Finite Element Methods Lecture Notes Winter Term 2017/18. R. Verfürth. Fakultät für Mathematik, Ruhr-Universität Bochum
Adaptive Finite Element Methods Lecture Notes Winter Term 2017/18 R. Verfürth Fakultät für Mathematik, Ruhr-Universität Bochum Contents Chapter I. Introduction 7 I.1. Motivation 7 I.2. Sobolev and finite
More informationVirtual Element Methods for general second order elliptic problems
Virtual Element Methods for general second order elliptic problems Alessandro Russo Department of Mathematics and Applications University of Milano-Bicocca, Milan, Italy and IMATI-CNR, Pavia, Italy Workshop
More informationPREPRINT 2010:23. A nonconforming rotated Q 1 approximation on tetrahedra PETER HANSBO
PREPRINT 2010:23 A nonconforming rotated Q 1 approximation on tetrahedra PETER HANSBO Department of Mathematical Sciences Division of Mathematics CHALMERS UNIVERSITY OF TECHNOLOGY UNIVERSITY OF GOTHENBURG
More informationInstitut de Recherche MAthématique de Rennes
LMS Durham Symposium: Computational methods for wave propagation in direct scattering. - July, Durham, UK The hp version of the Weighted Regularization Method for Maxwell Equations Martin COSTABEL & Monique
More informationNon-Conforming Finite Element Methods for Nonmatching Grids in Three Dimensions
Non-Conforming Finite Element Methods for Nonmatching Grids in Three Dimensions Wayne McGee and Padmanabhan Seshaiyer Texas Tech University, Mathematics and Statistics (padhu@math.ttu.edu) Summary. In
More informationETNA Kent State University
Electronic Transactions on Numerical Analysis. Volume 37, pp. 166-172, 2010. Copyright 2010,. ISSN 1068-9613. ETNA A GRADIENT RECOVERY OPERATOR BASED ON AN OBLIQUE PROJECTION BISHNU P. LAMICHHANE Abstract.
More informationConvergence Rates for AFEM: PDE on Parametric Surfaces
Department of Mathematics and Institute for Physical Science and Technology University of Maryland Joint work with A. Bonito and R. DeVore (Texas a&m) J.M. Cascón (Salamanca, Spain) K. Mekchay (Chulalongkorn,
More informationarxiv: v1 [math.na] 27 Jan 2016
Virtual Element Method for fourth order problems: L 2 estimates Claudia Chinosi a, L. Donatella Marini b arxiv:1601.07484v1 [math.na] 27 Jan 2016 a Dipartimento di Scienze e Innovazione Tecnologica, Università
More informationA Multigrid Method for Two Dimensional Maxwell Interface Problems
A Multigrid Method for Two Dimensional Maxwell Interface Problems Susanne C. Brenner Department of Mathematics and Center for Computation & Technology Louisiana State University USA JSA 2013 Outline A
More informationConstruction of wavelets. Rob Stevenson Korteweg-de Vries Institute for Mathematics University of Amsterdam
Construction of wavelets Rob Stevenson Korteweg-de Vries Institute for Mathematics University of Amsterdam Contents Stability of biorthogonal wavelets. Examples on IR, (0, 1), and (0, 1) n. General domains
More informationHierarchic Isogeometric Large Rotation Shell Elements Including Linearized Transverse Shear Parametrization
Proceedings of the 7th GACM Colloquium on Computational Mechanics for Young Scientists from Academia and Industry October 11-13, 2017 in Stuttgart, Germany Hierarchic Isogeometric Large Rotation Shell
More informationA Framework for Analyzing and Constructing Hierarchical-Type A Posteriori Error Estimators
A Framework for Analyzing and Constructing Hierarchical-Type A Posteriori Error Estimators Jeff Ovall University of Kentucky Mathematics www.math.uky.edu/ jovall jovall@ms.uky.edu Kentucky Applied and
More informationarxiv: v1 [cs.ce] 27 Dec 2018
ISOGEOMETRIC MORTAR COUPLING FOR ELECTROMAGNETIC PROBLEMS ANNALISA BUFFA, JACOPO CORNO, CARLO DE FALCO, SEBASTIAN SCHÖPS, AND RAFAEL VÁZQUEZ arxiv:1901.00759v1 [cs.ce] 27 Dec 2018 Abstract. This paper
More informationPREPRINT 2010:25. Fictitious domain finite element methods using cut elements: II. A stabilized Nitsche method ERIK BURMAN PETER HANSBO
PREPRINT 2010:25 Fictitious domain finite element methods using cut elements: II. A stabilized Nitsche method ERIK BURMAN PETER HANSBO Department of Mathematical Sciences Division of Mathematics CHALMERS
More informationMatrix assembly by low rank tensor approximation
Matrix assembly by low rank tensor approximation Felix Scholz 13.02.2017 References Angelos Mantzaflaris, Bert Juettler, Boris Khoromskij, and Ulrich Langer. Matrix generation in isogeometric analysis
More informationAND BARBARA I. WOHLMUTH
A QUASI-DUAL LAGRANGE MULTIPLIER SPACE FOR SERENDIPITY MORTAR FINITE ELEMENTS IN 3D BISHNU P. LAMICHHANE AND BARBARA I. WOHLMUTH Abstract. Domain decomposition techniques provide a flexible tool for the
More informationGoal. Robust A Posteriori Error Estimates for Stabilized Finite Element Discretizations of Non-Stationary Convection-Diffusion Problems.
Robust A Posteriori Error Estimates for Stabilized Finite Element s of Non-Stationary Convection-Diffusion Problems L. Tobiska and R. Verfürth Universität Magdeburg Ruhr-Universität Bochum www.ruhr-uni-bochum.de/num
More informationR T (u H )v + (2.1) J S (u H )v v V, T (2.2) (2.3) H S J S (u H ) 2 L 2 (S). S T
2 R.H. NOCHETTO 2. Lecture 2. Adaptivity I: Design and Convergence of AFEM tarting with a conforming mesh T H, the adaptive procedure AFEM consists of loops of the form OLVE ETIMATE MARK REFINE to produce
More informationAn axisymmetric PIC code based on isogeometric analysis
Author manuscript, published in "CEMRACS 2010, Marseille : France (2010" DOI : 10.1051/proc/2011016 An axisymmetric PIC code based on isogeometric analysis A. Back A. Crestetto A. Ratnani E. Sonnendrücker
More informationLocal discontinuous Galerkin methods for elliptic problems
COMMUNICATIONS IN NUMERICAL METHODS IN ENGINEERING Commun. Numer. Meth. Engng 2002; 18:69 75 [Version: 2000/03/22 v1.0] Local discontinuous Galerkin methods for elliptic problems P. Castillo 1 B. Cockburn
More informationChapter 6 A posteriori error estimates for finite element approximations 6.1 Introduction
Chapter 6 A posteriori error estimates for finite element approximations 6.1 Introduction The a posteriori error estimation of finite element approximations of elliptic boundary value problems has reached
More informationFinite element approximation of eigenvalue problems
Acta NumeTica (2010), pp. 1-120 doi: 10.1017/80962492910000012 Cambridge University Press, 2010 Finite element approximation of eigenvalue problems Daniele Boffi Dipartimento di Matematica, Universita
More informationA Posteriori Existence in Adaptive Computations
Report no. 06/11 A Posteriori Existence in Adaptive Computations Christoph Ortner This short note demonstrates that it is not necessary to assume the existence of exact solutions in an a posteriori error
More informationFind (u,p;λ), with u 0 and λ R, such that u + p = λu in Ω, (2.1) div u = 0 in Ω, u = 0 on Γ.
A POSTERIORI ESTIMATES FOR THE STOKES EIGENVALUE PROBLEM CARLO LOVADINA, MIKKO LYLY, AND ROLF STENBERG Abstract. We consider the Stokes eigenvalue problem. For the eigenvalues we derive both upper and
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University The Residual and Error of Finite Element Solutions Mixed BVP of Poisson Equation
More informationThe Mortar Wavelet Method Silvia Bertoluzza Valerie Perrier y October 29, 1999 Abstract This paper deals with the construction of wavelet approximatio
The Mortar Wavelet Method Silvia Bertoluzza Valerie Perrier y October 9, 1999 Abstract This paper deals with the construction of wavelet approximation spaces, in the framework of the Mortar method. We
More informationIntroduction. J.M. Burgers Center Graduate Course CFD I January Least-Squares Spectral Element Methods
Introduction In this workshop we will introduce you to the least-squares spectral element method. As you can see from the lecture notes, this method is a combination of the weak formulation derived from
More informationb i (x) u + c(x)u = f in Ω,
SIAM J. NUMER. ANAL. Vol. 39, No. 6, pp. 1938 1953 c 2002 Society for Industrial and Applied Mathematics SUBOPTIMAL AND OPTIMAL CONVERGENCE IN MIXED FINITE ELEMENT METHODS ALAN DEMLOW Abstract. An elliptic
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Numerical Methods for Partial Differential Equations Finite Difference Methods
More informationTrefftz-Discontinuous Galerkin Methods for the Time-Harmonic Maxwell Equations
Trefftz-Discontinuous Galerkin Methods for the Time-Harmonic Maxwell Equations Ilaria Perugia Dipartimento di Matematica - Università di Pavia (Italy) http://www-dimat.unipv.it/perugia Joint work with
More informationA LAGRANGE MULTIPLIER METHOD FOR ELLIPTIC INTERFACE PROBLEMS USING NON-MATCHING MESHES
A LAGRANGE MULTIPLIER METHOD FOR ELLIPTIC INTERFACE PROBLEMS USING NON-MATCHING MESHES P. HANSBO Department of Applied Mechanics, Chalmers University of Technology, S-4 96 Göteborg, Sweden E-mail: hansbo@solid.chalmers.se
More informationAdaptive Boundary Element Methods Part 1: Newest Vertex Bisection. Dirk Praetorius
CENTRAL School on Analysis and Numerics for PDEs November 09-12, 2015 Part 1: Newest Vertex Bisection Dirk Praetorius TU Wien Institute for Analysis and Scientific Computing Outline 1 Regular Triangulations
More informationSparse Tensor Galerkin Discretizations for First Order Transport Problems
Sparse Tensor Galerkin Discretizations for First Order Transport Problems Ch. Schwab R. Hiptmair, E. Fonn, K. Grella, G. Widmer ETH Zürich, Seminar for Applied Mathematics IMA WS Novel Discretization Methods
More informationBenchmarking high order finite element approximations for one-dimensional boundary layer problems
Benchmarking high order finite element approximations for one-dimensional boundary layer problems Marcello Malagù,, Elena Benvenuti, Angelo Simone Department of Engineering, University of Ferrara, Italy
More informationA Multiscale DG Method for Convection Diffusion Problems
A Multiscale DG Method for Convection Diffusion Problems Annalisa Buffa Istituto di Matematica Applicata e ecnologie Informatiche - Pavia National Research Council Italy Joint project with h. J.R. Hughes,
More informationThe Mortar Boundary Element Method
The Mortar Boundary Element Method A Thesis submitted for the degree of Doctor of Philosophy by Martin Healey School of Information Systems, Computing and Mathematics Brunel University March 2010 Abstract
More informationStochastic multiscale modeling of subsurface and surface flows. Part III: Multiscale mortar finite elements for coupled Stokes-Darcy flows
Stochastic multiscale modeling of subsurface and surface flows. Part III: Multiscale mortar finite elements for coupled Stokes-Darcy flows Ivan otov Department of Mathematics, University of Pittsburgh
More informationThe Virtual Element Method: an introduction with focus on fluid flows
The Virtual Element Method: an introduction with focus on fluid flows L. Beirão da Veiga Dipartimento di Matematica e Applicazioni Università di Milano-Bicocca VEM people (or group representatives): P.
More informationABHELSINKI UNIVERSITY OF TECHNOLOGY
ABHELSINKI UNIVERSITY OF TECHNOLOGY TECHNISCHE UNIVERSITÄT HELSINKI UNIVERSITE DE TECHNOLOGIE D HELSINKI A posteriori error analysis for the Morley plate element Jarkko Niiranen Department of Structural
More informationMultigrid Methods for Elliptic Obstacle Problems on 2D Bisection Grids
Multigrid Methods for Elliptic Obstacle Problems on 2D Bisection Grids Long Chen 1, Ricardo H. Nochetto 2, and Chen-Song Zhang 3 1 Department of Mathematics, University of California at Irvine. chenlong@math.uci.edu
More informationHybridized Discontinuous Galerkin Methods
Hybridized Discontinuous Galerkin Methods Theory and Christian Waluga Joint work with Herbert Egger (Uni Graz) 1st DUNE User Meeting, Stuttgart Christian Waluga (AICES) HDG Methods October 6-8, 2010 1
More informationMulti-level Bézier extraction for hierarchical local refinement of Isogeometric Analysis
Multi-level Bézier extraction for hierarchical local refinement of Isogeometric Analysis Davide D Angella a,b,, Stefan Kollmannsberger a, Ernst Rank a,b, Alessandro Reali b,c a Chair for Computation in
More informationISOGEOMETRIC BDDC PRECONDITIONERS WITH DELUXE SCALING TR
ISOGOMTRIC BDDC PRCONDITIONRS WITH DLUX SCALING L. BIRÃO DA VIGA, L.. PAVARINO, S. SCACCHI, O. B. WIDLUND, AND S. ZAMPINI TR2013-955 Abstract. A BDDC (Balancing Domain Decomposition by Constraints) preconditioner
More informationOn an Approximation Result for Piecewise Polynomial Functions. O. Karakashian
BULLETIN OF THE GREE MATHEMATICAL SOCIETY Volume 57, 010 (1 7) On an Approximation Result for Piecewise Polynomial Functions O. arakashian Abstract We provide a new approach for proving approximation results
More informationAxioms of Adaptivity (AoA) in Lecture 1 (sufficient for optimal convergence rates)
Axioms of Adaptivity (AoA) in Lecture 1 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and
More informationAxioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates)
Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and
More informationScientific Computing WS 2017/2018. Lecture 18. Jürgen Fuhrmann Lecture 18 Slide 1
Scientific Computing WS 2017/2018 Lecture 18 Jürgen Fuhrmann juergen.fuhrmann@wias-berlin.de Lecture 18 Slide 1 Lecture 18 Slide 2 Weak formulation of homogeneous Dirichlet problem Search u H0 1 (Ω) (here,
More informationNonstationary Subdivision Schemes and Totally Positive Refinable Functions
Nonstationary Subdivision Schemes and Totally Positive Refinable Functions Laura Gori and Francesca Pitolli December, 2007 Abstract In this paper we construct a class of totally positive refinable functions,
More informationMaximum norm estimates for energy-corrected finite element method
Maximum norm estimates for energy-corrected finite element method Piotr Swierczynski 1 and Barbara Wohlmuth 1 Technical University of Munich, Institute for Numerical Mathematics, piotr.swierczynski@ma.tum.de,
More informationRate optimal adaptive FEM with inexact solver for strongly monotone operators
ASC Report No. 19/2016 Rate optimal adaptive FEM with inexact solver for strongly monotone operators G. Gantner, A. Haberl, D. Praetorius, B. Stiftner Institute for Analysis and Scientific Computing Vienna
More informationANALYSIS OF THE FINITE ELEMENT METHOD FOR TRANSMISSION/MIXED BOUNDARY VALUE PROBLEMS ON GENERAL POLYGONAL DOMAINS
ANALYSIS OF THE FINITE ELEMENT METHOD FOR TRANSMISSION/MIXED BOUNDARY VALUE PROBLEMS ON GENERAL POLYGONAL DOMAINS HENGGUANG LI, ANNA MAZZUCATO, AND VICTOR NISTOR Abstract. We study theoretical and practical
More informationMimetic Finite Difference methods
Mimetic Finite Difference methods An introduction Andrea Cangiani Università di Roma La Sapienza Seminario di Modellistica Differenziale Numerica 2 dicembre 2008 Andrea Cangiani (IAC CNR) mimetic finite
More informationISOGEOMETRIC METHODS IN STRUCTURAL DYNAMICS AND WAVE PROPAGATION
COMPDYN 29 ECCOMAS Thematic Conference on Computational Methods in Structural Dynamics and Earthquake Engineering M. Papadrakakis, N.D. Lagaros, M. Fragiadakis (eds.) Rhodes, Greece, 22-24 June 29 ISOGEOMETRIC
More informationMesh Grading towards Singular Points Seminar : Elliptic Problems on Non-smooth Domain
Mesh Grading towards Singular Points Seminar : Elliptic Problems on Non-smooth Domain Stephen Edward Moore Johann Radon Institute for Computational and Applied Mathematics Austrian Academy of Sciences,
More informationRobust Domain Decomposition Preconditioners for Abstract Symmetric Positive Definite Bilinear Forms
www.oeaw.ac.at Robust Domain Decomposition Preconditioners for Abstract Symmetric Positive Definite Bilinear Forms Y. Efendiev, J. Galvis, R. Lazarov, J. Willems RICAM-Report 2011-05 www.ricam.oeaw.ac.at
More informationEFFICIENT MULTIGRID BASED SOLVERS FOR ISOGEOMETRIC ANALYSIS
6th European Conference on Computational Mechanics (ECCM 6) 7th European Conference on Computational Fluid Dynamics (ECFD 7) 1115 June 2018, Glasgow, UK EFFICIENT MULTIGRID BASED SOLVERS FOR ISOGEOMETRIC
More informationLocking phenomena in Computational Mechanics: nearly incompressible materials and plate problems
Locking phenomena in Computational Mechanics: nearly incompressible materials and plate problems C. Lovadina Dipartimento di Matematica Univ. di Pavia IMATI-CNR, Pavia Bologna, September, the 18th 2006
More informationBDDC deluxe for Isogeometric Analysis
BDDC deluxe for sogeometric Analysis L. Beirão da Veiga 1, L.. Pavarino 1, S. Scacchi 1, O. B. Widlund 2, and S. Zampini 3 1 ntroduction The main goal of this paper is to design, analyze, and test a BDDC
More informationA Least-Squares Finite Element Approximation for the Compressible Stokes Equations
A Least-Squares Finite Element Approximation for the Compressible Stokes Equations Zhiqiang Cai, 1 Xiu Ye 1 Department of Mathematics, Purdue University, 1395 Mathematical Science Building, West Lafayette,
More informationANALYSIS OF LAMINATED COMPOSITE PLATES USING ISOGEOMETRIC COLLOCATION METHOD
ECCOMAS Congress 0 VII European Congress on Computational Methods in Applied Sciences and Engineering M. Papadrakakis, V. Papadopoulos, G. Stefanou, V. Plevris eds.) Crete Island, Greece, 5 10 June 0 ANALYSIS
More informationBasic Concepts of Adaptive Finite Element Methods for Elliptic Boundary Value Problems
Basic Concepts of Adaptive Finite lement Methods for lliptic Boundary Value Problems Ronald H.W. Hoppe 1,2 1 Department of Mathematics, University of Houston 2 Institute of Mathematics, University of Augsburg
More informationQUASI-OPTIMAL CONVERGENCE RATE OF AN ADAPTIVE DISCONTINUOUS GALERKIN METHOD
QUASI-OPIMAL CONVERGENCE RAE OF AN ADAPIVE DISCONINUOUS GALERKIN MEHOD ANDREA BONIO AND RICARDO H. NOCHEO Abstract. We analyze an adaptive discontinuous finite element method (ADFEM) for symmetric second
More informationISOGEOMETRIC COLLOCATION METHOD FOR ELASTICITY PROBLEMS CONTAINING SINGULARITIES. Puja Rattan
ISOGEOMETRIC COLLOCATION METHOD FOR ELASTICITY PROBLEMS CONTAINING SINGULARITIES by Puja Rattan A dissertation proposal submitted to the faculty of The University of North Carolina at Charlotte in partial
More informationMapping Techniques for Isogeometric Analysis of Elliptic Boundary Value Problems Containing Singularities
Mapping Techniques for Isogeometric Analysis of Elliptic Boundary Value Problems Containing Singularities Jae Woo Jeong Department of Mathematics, Miami University, Hamilton, OH 450 Hae-Soo Oh Department
More informationModélisation d'interfaces linéaires et non linéaires dans le cadre X-FEM
Modélisation d'interfaces linéaires et non linéaires dans le cadre X-FEM Nicolas MOËS Ecole Centrale de Nantes, FRANCE GeM Institute - CNRS Journées Interface Numérique, GDR-IFS, CNAM, PARIS, 14-15 Mai
More informationarxiv: v2 [math.na] 17 Jun 2010
Numerische Mathematik manuscript No. (will be inserted by the editor) Local Multilevel Preconditioners for Elliptic Equations with Jump Coefficients on Bisection Grids Long Chen 1, Michael Holst 2, Jinchao
More informationCIMPA Summer School on Current Research in Finite Element Methods
CIMPA Summer School on Current Research in Finite Element Methods Local zooming techniques for the finite element method Alexei Lozinski Laboratoire de mathématiques de Besançon Université de Franche-Comté,
More informationA Nodal Spline Collocation Method for the Solution of Cauchy Singular Integral Equations 1
European Society of Computational Methods in Sciences and Engineering (ESCMSE) Journal of Numerical Analysis, Industrial and Applied Mathematics (JNAIAM) vol. 3, no. 3-4, 2008, pp. 211-220 ISSN 1790 8140
More informationR. M. Brown. 29 March 2008 / Regional AMS meeting in Baton Rouge. Department of Mathematics University of Kentucky. The mixed problem.
mixed R. M. Department of Mathematics University of Kentucky 29 March 2008 / Regional AMS meeting in Baton Rouge Outline mixed 1 mixed 2 3 4 mixed We consider the mixed boundary value Lu = 0 u = f D u
More informationSome New Elements for the Reissner Mindlin Plate Model
Boundary Value Problems for Partial Differential Equations and Applications, J.-L. Lions and C. Baiocchi, eds., Masson, 1993, pp. 287 292. Some New Elements for the Reissner Mindlin Plate Model Douglas
More informationSpace-time isogeometric analysis of parabolic evolution equations
www.oeaw.ac.at Space-time isogeometric analysis of parabolic evolution equations U. Langer, S.E. Moore, M. Neumüller RICAM-Report 2015-19 www.ricam.oeaw.ac.at SPACE-TIME ISOGEOMETRIC ANALYSIS OF PARABOLIC
More informationarxiv: v1 [math.na] 5 Jun 2018
PRIMAL-DUAL WEAK GALERKIN FINIE ELEMEN MEHODS FOR ELLIPIC CAUCHY PROBLEMS CHUNMEI WANG AND JUNPING WANG arxiv:1806.01583v1 [math.na] 5 Jun 2018 Abstract. he authors propose and analyze a well-posed numerical
More informationBases of T-meshes and the refinement of hierarchical B-splines
arxiv:1401.7076v1 [cs.cg] 28 Jan 2014 Bases of T-meshes and the refinement of hierarchical B-splines Dmitry Berdinsky Tae-wan Kim Durkbin Cho Cesare Bracco Sutipong Kiatpanichgij Abstract. In this paper
More informationNumerical methods for PDEs FEM convergence, error estimates, piecewise polynomials
Platzhalter für Bild, Bild auf Titelfolie hinter das Logo einsetzen Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials Dr. Noemi Friedman Contents of the course Fundamentals
More informationBETI for acoustic and electromagnetic scattering
BETI for acoustic and electromagnetic scattering O. Steinbach, M. Windisch Institut für Numerische Mathematik Technische Universität Graz Oberwolfach 18. Februar 2010 FWF-Project: Data-sparse Boundary
More informationTrefftz-discontinuous Galerkin methods for time-harmonic wave problems
Trefftz-discontinuous Galerkin methods for time-harmonic wave problems Ilaria Perugia Dipartimento di Matematica - Università di Pavia (Italy) http://www-dimat.unipv.it/perugia Joint work with Ralf Hiptmair,
More information