Abstract
The scale-dependent homogenization is applied to a hyperbolic thermoelastic material with two relaxation times, where conductivity and stiffness are wide-sense stationary ergodic random fields. The previously established scaling functions for the Fourier-type conductivity and linear elastic responses are used to describe the trends to scale from the mesoscale statistical volume element level (SVE) to the (representative volume element) RVE level of a deterministic homogeneous continuum. In the case of white-noise type random fields, this finite-size scaling can be quantified via universally appearing stretched exponentials for conductivity and elasticity problems.
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Acknowledgements
Comments of two anonymous reviewers helped improve this note. The work was supported by the RDECOM-AMSAA: Army Materiel Systems Analysis Activity (William Davis) under the auspices of the US Army Research Office Scientific Services Program administered by Battelle (W911NF-11-D-0001 DO# 0169; TCN 12-078).
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Ostoja-Starzewski, M., Costa, L. & Ranganathan, S.I. Scale-Dependent Homogenization of Random Hyperbolic Thermoelastic Solids. J Elast 118, 243–250 (2015). https://doi.org/10.1007/s10659-014-9483-4
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DOI: https://doi.org/10.1007/s10659-014-9483-4
Keywords
- Finite-size scaling
- Homogenization
- Hyperbolic thermoelasticity
- Random fields
- Relaxation times
- Representative volume element
- Statistical volume element
- Stretched exponentials