% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Vasechko:808671,
      author       = {Vasechko, V. and Pecanac, G. and Kuhn, Bernd and
                      Malzbender, Jürgen},
      title        = {{M}echanical {P}roperties of {P}orous {ITM} {A}lloy},
      journal      = {International journal of hydrogen energy},
      volume       = {41},
      issn         = {0360-3199},
      address      = {New York, NY [u.a.]},
      publisher    = {Elsevier},
      reportid     = {FZJ-2016-02304},
      pages        = {562-569},
      year         = {2016},
      abstract     = {Mechanical characteristics of porous ITM are assessed for
                      the use as metallic substrate in solid oxide fuel cell
                      stacks. Elastic modulus and Poisson's ratio are determined
                      using an impulse excitation technique, thermal expansion is
                      measured with an optical dilatometer, and ultimate tensile
                      strength and creep are measured in a tensile set-up. Data
                      are compared and discussed with respect to the properties of
                      dense ITM. The results indicate that the coefficient of
                      thermal expansion is not affected by the porosity, while the
                      Poisson's ratio is only affected to a minor extent. The
                      coefficient of thermal expansion and elastic modulus appear
                      to be influenced by a ferromagnetic-paramagnetic transition.
                      The elastic modulus of the porous material is, as expected,
                      reduced due to smaller effective area of the porous
                      specimens. The largest change compared to the behavior
                      observed for the dense ITM is seen for the ultimate tensile
                      strength. The large creep stress exponent of the dense and
                      porous material over a wide stress range is a result of the
                      dispersed nano-sized Y-rich phase, however,},
      cin          = {IEK-2},
      ddc          = {660},
      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:000368955300059},
      doi          = {10.1016/j.ijhydene.2015.10.075},
      url          = {https://juser.fz-juelich.de/record/808671},
}