Abstract For polyhedral constrained optimization problems and a feasible point$$\textbf{x}$$ , it is shown that the projection of the negative gradient on the tangent cone, denoted$$\nabla _\varOmega f(\textbf{x})$$ , has an orthogonal decomposition of the form$$\varvec{\beta }(\textbf{x}) + \varvec{\varphi }(\textbf{x})$$ . At a stationary point,$$\nabla _\varOmega f(\textbf{x}) = \textbf{0}$$ so$$\Vert \nabla _\varOmega f(\textbf{x})\Vert $$ reflects the distance to a stationary point. Away from a stationary point,$$\Vert \varvec{\beta }(\textbf{x})\Vert $$ and$$\Vert \varvec{\varphi }(\textbf{x})\Vert $$ measure different aspects of optimality since$$\varvec{\beta }(\textbf{x})$$ only vanishes when the KKT multipliers at$$\textbf{x}$$ have the correct sign, while$$\varvec{\varphi }(\textbf{x})$$ only vanishes when$$\textbf{x}$$ is a stationary point in the active manifold. As an application of the theory, an active set algorithm is developed for convex quadratic programs which adapts the flow of the algorithm based on a comparison between$$\Vert \varvec{\beta }(\textbf{x})\Vert $$ and$$\Vert \varvec{\varphi }(\textbf{x})\Vert $$ .
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Controllable deformations in compressible isotropic implicit elasticity
Abstract For a given material,controllable deformationsare those deformations that can be maintained in the absence of body forces and by applying only boundary tractions. For a given class of materials,universal deformationsare those deformations that are controllable for any material within the class. In this paper, we characterize the universal deformations in compressible isotropic implicit elasticity defined by solids whose constitutive equations, in terms of the Cauchy stress$$\varvec{\sigma }$$ and the left Cauchy-Green strain$$\textbf{b}$$ , have the implicit form$$\varvec{\textsf{f}}(\varvec{\sigma },\textbf{b})=\textbf{0}$$ . We prove that universal deformations are homogeneous. However, an important observation is that, unlike Cauchy (and Green) elasticity, not every homogeneous deformation is constitutively admissible for a given implicit-elastic solid. In other words, the set of universal deformations is material-dependent, yet it remains a subset of homogeneous deformations.
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- Award ID(s):
- 1939901
- PAR ID:
- 10536215
- Publisher / Repository:
- Springer Science + Business Media
- Date Published:
- Journal Name:
- Zeitschrift für angewandte Mathematik und Physik
- Volume:
- 75
- Issue:
- 5
- ISSN:
- 0044-2275
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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