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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Gueguen, Yann
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (28/28 displayed)
- 2024Effect of calcium and potassium oxide addition on the viscosity and fragility of a calcium aluminosilicate meltcitations
- 2021Non-equilibrium viscoelastic behavior of chalcogenide glass fibers
- 2020Mechanics and physics of a glass/particles photonic spongecitations
- 2020Viscoelastic analysis of RFDA measurements applied to oxide glassescitations
- 2020Viscoelastic analysis of RFDA measurements applied to oxide glassescitations
- 2020Deformation of a chalcogenide glass film under optical modulated excitationcitations
- 2018Fracture toughness, fracture energy and slow crack growth of glass as investigated by the Single-Edge Precracked Beam (SEPB) and Chevron-Notched Beam (CNB) methodscitations
- 2018Fracture toughness, fracture energy and slow crack growth of glass as investigated by the Single-Edge Precracked Beam (SEPB) and Chevron-Notched Beam (CNB) methodscitations
- 2017Rheology of chalcogenide glasses under light irradiation
- 2017Molecular design of melt-spinnable co-polymers as Si–B–C–N fiber precursorscitations
- 2017Mechanical model of giant photoexpansion in a chalcogenide glass and the role of photofluiditycitations
- 2017Co-sputtered amorphous Ge-Sb-Se thin films: Optical properties and structurecitations
- 2016Elasticity and viscosity of BaO-TiO2-SiO2 glasses in the 0.9 to 1.2T(g) temperature intervalcitations
- 2015A relationship between non-exponential stress relaxation and delayed elasticity in the viscoelastic process in amorphous solids: Illustration on a chalcogenide glasscitations
- 2015A relationship between non-exponential stress relaxation and delayed elasticity in the viscoelastic process in amorphous solids: Illustration on a chalcogenide glasscitations
- 2013Physical properties of the GexSe1 − x glasses in the 0 < x < 0.42 range in correlation with their structurecitations
- 2012Photoinduced Fluidity and Viscoelasticity in Chalcogenide Glassescitations
- 2012Fragile-strong behavior in the AsxSe1-x glass forming system in relation to structural dimensionalitycitations
- 2012Investigation of the Mechanisms Involved in the Sintering of Chalcogenide Glasses and the Preparation of Glass-Ceramics by Spark Plasma Sinteringcitations
- 2011Assessment of rheological and thermodynamic properties of the Pd40Ni40P20 bulk metallic glass around glass transition using an indentation creep techniquecitations
- 2010Correlation between structure and physical properties of chalcogenide glasses in the AsxSe1-x systemcitations
- 2010Optical microfabrication of tapers in low-loss chalcogenide fiberscitations
- 2010Photoinduced fluidity in chalcogenide glasses at low and high intensities: A model accounting for photon efficiencycitations
- 2009Correlation Between Thermal and Mechanical Relaxation in Chalcogenide Glass Fiberscitations
- 2009Influence of ageing conditions on the mechanical properties of Te-As-Se fibrescitations
- 2008Sub-Tg viscoelastic behaviour of chalcogenide glasses, anomalous viscous flow and stress relaxationcitations
- 2008Temperature dependence of mechanical properties and pressure sensitivity in metallic glasses below glass transitioncitations
- 2008Temperature dependence of mechanical properties and pressure sensitivity in metallic glasses below glass transitioncitations
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article
A relationship between non-exponential stress relaxation and delayed elasticity in the viscoelastic process in amorphous solids: Illustration on a chalcogenide glass
Abstract
Inorganic glasses are viscoelastic materials since they exhibit, below as well as above their glass transition temperature, a viscoelas-tic deformation under stress, which can be decomposed into a sum of an elastic part, an inelastic (or viscous) part and a delayed elastic part. The delayed elastic part is responsible for the non-linear primary creep stage observed during creep tests. During a stress relaxation test, the strain, imposed, is initially fully elastic, but is transformed, as the stress relaxes, into an inelastic and a delayed elastic strains. For linear viscoelastic materials, if the stress relaxation function can be fitted by a stretched exponential function, the evolution of each part of the strain can be predicted using the Boltzmann superposition principle. We develop here the equations of these evolutions, and we illustrate their accuracy by comparing them with experimental evolutions measured on GeSe 9 glass fibers. We illustrate also, by simple equations, the relationship between any kind of relaxation function based on additive contribution of different relaxation processes and the delayed elastic contribution to stress relaxation: the delayed elasticity is directly correlated to the dispersion of relaxations times of the processes involved during relaxation.