Jean-Baptiste Leblond

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Jean-Baptiste Leblond (born 21 May 1957 in Boulogne-Billancourt) is a French materials scientist, member of the Mechanical Modelling Laboratory of the Pierre-et-Marie-Curie University (MISES) and professor at the same university. [1]

Contents

Biography

Leblond attended his scientific preparatory classes, notably in the special M' mathematics class at the Lycée Louis-le-Grand and was admitted to the École normale supérieure de la rue d'Ulm, mathematics option, in 1976. He then joined the Corps des mines and became a doctor of physical sciences.

Since 2005, he has been a member of the French Academy of Sciences [2] and a founding member of the French Academy of Technologies (2000). [3] He is a senior member of the Institut universitaire de France.

Scientific fields covered

Leblond's kinetic theory

This is an approach established by Leblond in his work on phase transformations.

The theory proposes an evolutionary model to quantify the composition of the different phases of a crystalline material during heat treatment.

The method is based on experimentally established CRT (Continuous Cooling Transformation) diagrams to compose TTT (Time-Temperature-Transformation) diagrams, which are widely used for numerical simulation or for the manufacture of industrial parts.

The theory posits the equivalent volume fraction of a constituent yeq as the stationary solution of the evolution equations describing the phase change kinetics:

stationnart phase

We then suppose in anisothermal condition that the real fraction y is close to yeq, it is then possible to approximate the real value Y by a Taylor development at order 1:

The evolution is given by :

τ is determined on the one hand by the incubation period (critical time) and on the other hand by the cooling rates T.

There are also other formalisms such as the theory of Kirkaldy, Johnson-Mehl-Avrami or Waeckel. One of the most classical, quite old, is that of Johnson-Mehl-Avrami. The model proposed by Jean-Baptiste Leblod is in fact based on this classical model by generalizing it on two points: 1) it considers any number of phases and transformations between these phases, and not just two phases and a single transformation; 2) the transformations can remain, after an infinitely long time, partial, and not necessarily complete as in the Johnson-Mehl-Avrami model (this is linked to the existence, in the new model, of fractions "at equilibrium" of the phases towards which the system evolves after an infinite time, not necessarily equal to 0 or 1 but which can take any value between these limits).

The Leblond model is designed for applications in the thermometallurgical treatment of steels; this explains its success with the modellers of these treatments.

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References

  1. "Site internet JB Leblond".
  2. "Académie des sciences".
  3. "Académie des technologies".[ permanent dead link ]
  4. J.B. Leblond, J. Devaux, « A new kinetic model for anisothermal metallurgical transformations in steels including effect of austenite grain size », Acta Metallurgica, 32, 1984, p. 137-146
  5. J.B. Leblond, J. Devaux, J.C. Devaux, « Mathematical modelling of transformation plasticity in steels - I: Case of ideal-plastic phases », International Journal of Plasticity, 5, 1989, p. 551-572
  6. Y. El Majaty J.B. Leblond, D. Kondo, « A novel treatment of Greenwood-Johnson's mechanism of transformation plasticity - Case of spherical growth of nuclei of daughter-phase », Journal of the Mechanics and Physics of Solids, 121, 2018, p. 175-197
  7. J.B. Leblond, H.A. El-Sayed, J.M. Bergheau, « On the incorporation of surface tension in finite element calculations », Comptes Rendus Mécanique, 341, 2013, p. 770-775
  8. Y. Saadlaoui E. Feulvarch; A. Delache; J.B. Leblond; J.M. Bergheau (2018). "A new strategy for the numerical modeling of a weld pool". Comptes Rendus Mécanique (in French). 346 (11): 999–1017. Bibcode:2018CRMec.346..999S. doi: 10.1016/j.crme.2018.08.007 .
  9. J.B. Leblond, A. Karma, V. Lazarus, « Theoretical analysis of crack front instability in mode I+III », Journal of the Mechanics and Physics of Solids, 59, 2011, p. 1872-1887
  10. M. Gologanu, J.B. Leblond, J. Devaux, « Approximate models for ductile metals containing non-spherical voids - Case of axisymmetric prolate ellipsoidal cavities », Journal of the Mechanics and Physics of Solids, 41, 1993, p. 1723-1754
  11. M. Gologanu, J.B. Leblond, G. Perrin, J. Devaux, Recent extensions of Gurson's model for porous ductile metals, in: Continuum Micromechanics, P. Suquet, ed., Springer-Verlag, 1997, p. 61-130
  12. L. Morin, J.B. Leblond, V. Tvergaard, « Application of a model of plastic porous materials including void shape effects to the prediction of ductile failure under shear-dominated loadings », Journal of the Mechanics and Physics of Solids, 94, 2016, p. 148-166
  13. A. Benzerga, J.B. Leblond, A. Needleman, V. Tvergaard, « Ductile failure modeling », International Journal of Fracture, 201, 2016, p. 29-80
  14. J.B. Leblond, « A note on a nonlinear variant of Wagner's model of internal oxidation », Oxidation of Metals, 75, 2011, p. 93-101
  15. J.B. Leblond, J.M. Bergheau, R. Lacroix, D. Huin, « Implementation and application of some nonlinear models of diffusion/reaction in solids », Finite Elements in Analysis and Design, 1, 32, 2017, p. 8-26