1991
DOI: 10.1137/0522012
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Analysis and Computation of Symmetry-Breaking Bifurcation and Scaling Laws Using Group-Theoretic Methods

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Cited by 38 publications
(29 citation statements)
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“…Independently, Healey and his students [21][22][23][24], motivated by examples in structural mechanics, and Aston [25,26], motivated by a problem in water waves, developed similar theories but which allowed for infinite groups. An important idea is that, under the action of a group and for an appropriately chosen basis, the Jacobian of a non-linear problem 'block-diagonalizes', with consequent savings for numerical algorithms, and improved theoretical understanding [20,23,26]. Many of the group theoretic ideas can appear complicated, and one aim of this paper is to explain them as simply as possible for the O(2) group, which is relevant for many problems defined on a cylindrical domain.…”
Section: Introductionmentioning
confidence: 93%
“…Independently, Healey and his students [21][22][23][24], motivated by examples in structural mechanics, and Aston [25,26], motivated by a problem in water waves, developed similar theories but which allowed for infinite groups. An important idea is that, under the action of a group and for an appropriately chosen basis, the Jacobian of a non-linear problem 'block-diagonalizes', with consequent savings for numerical algorithms, and improved theoretical understanding [20,23,26]. Many of the group theoretic ideas can appear complicated, and one aim of this paper is to explain them as simply as possible for the O(2) group, which is relevant for many problems defined on a cylindrical domain.…”
Section: Introductionmentioning
confidence: 93%
“…In the sequel we consider the numerical approximation of the corresponding steady state problem and investigate its linear stability. With this in mind, employing the continuity equation (5.2), we rewrite the steady NavierStokes equations in the following divergence form (to facilitate the DG discretization): find u 0 and p 0 such that 6) subject to the boundary conditions outlined in (5.3)-(5.4) above, with u and p replaced by u 0 and p 0 , respectively. Here, for vectors v ∈ R m and w ∈ R n , m, n ≥ 1, the matrix v ⊗ w ∈ R m×n is the standard outer product defined by (v ⊗ w) kl = v k w l .…”
Section: Incompressible Navier-stokes Equationsmentioning
confidence: 99%
“…Aston [6]. Thereby, for u ∈ V s , the Jacobian operator F ′ u (u, λ; ·) has a diagonal block structure; more precisely, the following result holds.…”
mentioning
confidence: 96%
“…see Aston [5]. Thereby, for u ∈ V O(2) , our Jacobian operator F ′ u (u, λ; ·) has a diagonal block structure; more precisely the following result holds.…”
mentioning
confidence: 95%
“…It is a standard result, see Aston [5], that, for the O(2) case, there exists a unique orthogonal decomposition of V , namely,…”
mentioning
confidence: 99%