Pierre Suquet (born 22 October 1954) is a French theoretician mechanic and research director at the CNRS. He is a member of the French Academy of Sciences. [1]
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He did his preparatory classes in Grenoble (Maths Sup) then at Louis-Le Grand (Maths Spé), to join the École Normale Supérieure (1973) to become an agrégé de Mathématiques in 1975, and Doctor in 1982.
From 1983 to 1988 he was Professor at the University of Montpellier. Then CNRS Research Director, Mechanics and Acoustics Laboratory in Marseille, where he was Director from 1993 to 1999. From 2000 to 2001 he was Visiting Professor at the Clarke Millikan of the California Institute of Technology.
Pierre Suquet is a specialist in continuous media and the behaviour of solid materials. His main research interests are elastoplastic structures, homogenization of non-linear composites and numerical simulation in materials mechanics.
In 1978, Pierre Suquet introduced the space of vector fields with bounded deformation [2] [3] and established certain properties (existence of internal and external traces on any surface, compact injection...). It shows that the evolution problem for a perfectly plastic elastic body admits a solution in speed (of displacement) in this space under a safe loading condition. It shows that there can be an infinite number of solutions, regular or non-regular. [4] [5]
The framework of generalized standard environments, due to Helphen and Nguyen Quoc Son, allows an easy writing of the laws of macroscopic behaviour. [6] In 1982, Pierre Suquet [7] established homogenization results for environments characterized by 2 potentials (free energy and dissipation potentials) and showed in particular that the generalized standard structure is preserved by changing scales when geometric variations are neglected. [8] He notes that the homogenization of short-memory viscoelastic composites can lead to the appearance of long memory effects (an effect already noted by J. & E. Sanchez-Palencia in 1978). More recently, properties of these long memories have been established in relation to order moments 1 and 2 of the local fields.
In 1983, Pierre Suquet [9] gave a first upper bound of the resistance domain of a heterogeneous medium by solving a boundary analysis problem on a base cell. This result is improved by Bouchitte and Suquet [10] who show that the homogenized analysis problem is divided into two sub-problems, one purely volumetric for which the resistance domain is that given by the boundary analysis of a base cell, the second, surface area for which a surface homogenization problem (and not on unit cell) must be solved.
In 1993, Pierre Suquet [11] proposed a series of bollards for non-linear phase composites, using a method different from those available at the time (Willis, 1988, Ponte Castañeda, 1991), then showed in 1995 [12] [13] that Ponte Castañeda's (1991) variational method is a secant method using the second moment by phase of local fields.
In 1994, H. Moulinec and P. Suquet [14] [15] [16] [17] introduced a numerical method using massively the Fast Fourier Transform (FFT) using only a pixelized image of the study microstructure (without mesh size). By introducing a homogeneous reference medium, the heterogeneity of the medium is transformed into a polarization constraint. The Green operator of the reference medium, known explicitly in Fourier space, can be used to iteratively update the polarization field. Several improvements and accelerations have been made to this method, which is now used internationally in dedicated codes.
Since 2003, J.C. Michel and P. Suquet [18] [19] have been developing a method to reduce the number of internal variables of homogenized behavioural laws. This Nonuniform Transformation Field Analysis (NTFA) model uses the structuring of microscopic plastic deformation fields. A mode base is first built by the "snapshot POD" method along learning paths. Then the reduced kinetic equations for the field components in these modes are constructed by approaching the effective potentials by techniques derived from non-linear homogenization.
Solid mechanics is the branch of continuum mechanics that studies the behavior of solid materials, especially their motion and deformation under the action of forces, temperature changes, phase changes, and other external or internal agents.
Micromechanics is the analysis of composite or heterogeneous materials on the level of the individual constituents that constitute these materials.
This is an alphabetical list of articles pertaining specifically to Engineering Science and Mechanics (ESM). For a broad overview of engineering, please see Engineering. For biographies please see List of engineers and Mechanicians.
In the theory of composite materials, the representative elementary volume (REV) is the smallest volume over which a measurement can be made that will yield a value representative of the whole. In the case of periodic materials, one simply chooses a periodic unit cell, but in random media, the situation is much more complicated. For volumes smaller than the RVE, a representative property cannot be defined and the continuum description of the material involves Statistical Volume Element (SVE) and random fields. The property of interest can include mechanical properties such as elastic moduli, hydrogeological properties, electromagnetic properties, thermal properties, and other averaged quantities that are used to describe physical systems.
In mathematics, a function of bounded deformation is a function whose distributional derivatives are not quite well-behaved-enough to qualify as functions of bounded variation, although the symmetric part of the derivative matrix does meet that condition. Thought of as deformations of elasto-plastic bodies, functions of bounded deformation play a major role in the mathematical study of materials, e.g. the Francfort-Marigo model of brittle crack evolution.
Philippe G. Ciarlet is a French mathematician, known particularly for his work on mathematical analysis of the finite element method. He has contributed also to elasticity, to the theory of plates and shells and differential geometry.
Junuthula N. Reddy is a Distinguished Professor, Regent's Professor, and inaugural holder of the Oscar S. Wyatt Endowed Chair in Mechanical Engineering at Texas A&M University, College Station, Texas, USA.[1] He is an authoritative figure in the broad area of mechanics and one of the researchers responsible for the development of the Finite Element Method (FEM). He has made significant seminal contributions in the areas of finite element method, plate theory, solid mechanics, variational methods, mechanics of composites, functionally graded materials, fracture mechanics, plasticity, biomechanics, classical and non-Newtonian fluid mechanics, and applied functional analysis. Reddy has over 620 journal papers and 20 books and has given numerous national and international talks. He served as a member of the International Advisory Committee at ICTACEM, in 2001 and keynote addressing in 2014.[2][3]
In mathematics and physics, homogenization is a method of studying partial differential equations with rapidly oscillating coefficients, such as
João Arménio Correia Martins was born on November 11, 1951, at the southern town of Olhão in Portugal. He attended high school at the Liceu Nacional de Faro which he completed in 1969. Afterwards João Martins moved to Lisbon where he was graduate student of Civil Engineering at Instituto Superior Técnico (IST) until 1976. He was a research assistant and assistant instructor at IST until 1981. Subsequently, he entered the graduate school in the College of Engineering, Department of Aerospace Engineering and Engineering Mechanics of The University of Texas at Austin, USA. There he obtained a MSc in 1983 with a thesis titled A Numerical Analysis of a Class of Problems in Elastodynamics with Friction Effects and a PhD in 1986 with a thesis titled Dynamic Frictional Contact Problems Involving Metallic Bodies, both supervised by Prof. John Tinsley Oden. He returned to Portugal in 1986 and became assistant professor at IST. In 1989 he became associate professor and in 1996 he earned the academic degree of “agregado” from Universidade Técnica de Lisboa. Later, in 2005, he became full professor in the Department of Civil Engineering and Architecture of IST.
According to the classical theories of elastic or plastic structures made from a material with non-random strength (ft), the nominal strength (σN) of a structure is independent of the structure size (D) when geometrically similar structures are considered. Any deviation from this property is called the size effect. For example, conventional strength of materials predicts that a large beam and a tiny beam will fail at the same stress if they are made of the same material. In the real world, because of size effects, a larger beam will fail at a lower stress than a smaller beam.
The William Prager Medal is an award given annually by the Society of Engineering Science (SES) to an individual for "outstanding research contributions in either theoretical or experimental Solid Mechanics or both". This medal was established in 1983. The actual award is a medal with William Prager's likeness on one side and an honorarium of US$2000.
Johannes Ferdinand "Hans" Besseling was professor emeritus of Engineering Mechanics at the Delft University of Technology, worked in the field of the application of solid mechanics to the analysis of structures; constitutive equations for the mathematical description of material behaviour. His specialities are finite element methods, continuum thermodynamics, creep and plasticity of metals.
Leonid Berlyand is a Soviet and American mathematician, a professor of Penn State University. He is known for his works on homogenization, Ginzburg–Landau theory, mathematical modeling of active matter and mathematical foundations of deep learning.
Variational Asymptotic Method (VAM) is a powerful mathematical approach to simplify the process of finding stationary points for a described functional by taking advantage of small parameters. VAM is the synergy of variational principles and asymptotic approaches. Variational principles are applied to the defined functional as well as the asymptotes are applied to the same functional instead of applying on differential equations which is more prone error. This methodology is applicable for a whole range of physics problems, where the problem has to be defined in a variational form and should be able to identify the small parameters within the problem definition. In other words, VAM can be applicable where the functional is so complex in determining the stationary points either by analytical or by computationally expensive numerical analysis with an advantage of small parameters. Thus, approximate stationary points in the functional can be utilized to obtain the original functional.
Jean Salençon is a French physicist born on November 13, 1940. He is a member of the French Academy of Sciences and the French Academy of Technologies.
A number of processes of surface growth in areas ranging from mechanics of growing gravitational bodies through propagating fronts of phase transitions, epitaxial growth of nanostructures and 3D printing, growth of plants, and cell mobility require non-Euclidean description because of incompatibility of boundary conditions and different mechanisms of developing stresses at interfaces. Indeed, these mechanisms result in the curving of initially flat elements of the body and changing separation between different elements of it. Gradual accumulation of deformations under the influx of accumulating mass results in the memory-conscious grows of the body and makes strains the subject of long-range forces. As a result of all above factors, generic non-Euclidean growth is described in terms of Riemannian geometry with a space- and time-dependent curvature.
Jean-Baptiste Leblond, born on 21 May 1957 in Boulogne-Billancourt, is a materials scientist, member of the Mechanical Modelling Laboratory of the Pierre-et-Marie-Curie University (MISES) and professor at the same university.
André Zaoui is a French physicist in material mechanics, born on 8 June 1941. He is a corresponding member of the French Academy of sciences and a member of the French Academy of Technologies.
Leonid Isakovich Manevitch was a Soviet and Russian physicist, mechanical engineer, and mathematician. He made fundamental contributions to areas of nonlinear dynamics, composite and polymer physics, and asymptotology.
Crystal plasticity is a mesoscale computational technique that takes into account crystallographic anisotropy in modelling the mechanical behaviour of polycrystalline materials. The technique has typically been used to study deformation through the process of slip, however, there are some flavors of crystal plasticity that can incorporate other deformation mechanisms like twinning and phase transformations. Crystal plasticity is used to obtain the relationship between stress and strain that also captures the underlying physics at the crystal level. Hence, it can be used to predict not just the stress-strain response of a material, but also the texture evolution, micromechanical field distributions, and regions of strain localisation. The two widely used formulations of crystal plasticity are the one based on the finite element method known as Crystal Plasticity Finite Element Method (CPFEM), which is developed based on the finite strain formulation for the mechanics, and a spectral formulation which is more computationally efficient due to the fast Fourier transform, but is based on the small strain formulation for the mechanics.