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@ARTICLE{Fleck:862187,
      author       = {Fleck, M. and Ta, N. and Yin, Xiaoyan and Wang, Kai and
                      Hüter, Claas},
      title        = {{E}lastically {I}nduced {P}attern {F}ormation in the
                      {I}nitial and {F}rustrated {G}rowth {R}egime of {B}ainitic
                      {S}ubunits},
      journal      = {AIMS Materials Science},
      volume       = {6},
      number       = {1},
      issn         = {2372-0484},
      address      = {Springfield, Mo.},
      publisher    = {AIMS Press},
      reportid     = {FZJ-2019-02535},
      pages        = {52 - 62},
      year         = {2019},
      abstract     = {We present analytical and numerical results for the
                      dominant mechanisms of pattern selection in two growth
                      regimes which are crucial in elastically influenced
                      solid-solid transformations like the bainitic one. The first
                      growth regime comprises the very early regime, when in a
                      nucleation scenario the size of the nucleus is so small that
                      the bulk crystal structure is typically not yet fully
                      developed and the phase is elastically softened. Here we see
                      a dominant effect of curvature effects in analogy to the
                      theory on growth of lenticular melt inclusions. The second
                      growth regime is of specific interest to bainitic steels.
                      During the bainitic reaction subunits form, grow up to a
                      point where the thermodynamic driving force is kinetically
                      overcome by a deformation-induced growth barrier, stop
                      growth and then nucleate new subunits. Thus, the regime
                      prior to the new subunit nucleation corresponds to the
                      limiting case of vanishing growth velocity. For both,
                      analytical and numerical approach, we use sharp interface
                      descriptions of the problem, for the numerical approach we
                      invoke a representation of the problem in terms of boundary
                      integral equations.},
      cin          = {IEK-2},
      ddc          = {620},
      cid          = {I:(DE-Juel1)IEK-2-20101013},
      pnm          = {111 - Efficient and Flexible Power Plants (POF3-111)},
      pid          = {G:(DE-HGF)POF3-111},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000460760700005},
      doi          = {10.3934/matersci.2019.1.52},
      url          = {https://juser.fz-juelich.de/record/862187},
}