The role of water in the behavior of wood

Wood, due to its biological origin, has the capacity to interact with water. Sorption/desorption of moisture is accompanied with swelling/shrinkage and softening/hardening of its stiffness. The correct prediction of the behavior of wood components undergoing environmental loading requires that the moisture behavior and mechanical behavior of wood are considered in a coupled manner. We propose a comprehensive framework using a fully coupled poromechanical approach, where its multiscale implementation provides the capacity to take into account, directly, the exact geometry of the wood cellular structure, using computational homogenization. A hierarchical model is used to take into account the subcellular composite-like organization of the material. Such advanced modeling requires high-resolution experimental data for the appropriate determination of inputs and for its validation. High-resolution x-ray tomography, digital image correlation, and neutron imaging are presented as valuable methods to provide the required information.

[1]  Dominique Derome,et al.  Hysteretic swelling of wood at cellular scale probed by phase-contrast X-ray tomography. , 2011, Journal of structural biology.

[2]  I. D. Cave Modelling moisture-related mechanical properties of wood Part I: Properties of the wood constituents , 1978, Wood Science and Technology.

[3]  J. Carmeliet,et al.  Visualization and quantification of liquid water transport in softwood by means of neutron radiography , 2012 .

[4]  J. Carmeliet,et al.  Variation of measured cross-sectional cell dimensions and calculated water vapor permeability across a single growth ring of spruce wood , 2011, Wood Science and Technology.

[5]  C. C. Chamis,et al.  Simplified composite micromechanics equations for hygral, thermal and mechanical properties , 1983 .

[6]  V. Cnudde,et al.  UGCT: New X-ray radiography and tomography facility , 2007 .

[7]  J. Carmeliet,et al.  Computational up-scaling of anisotropic swelling and mechanical behavior of hierarchical cellular material , 2012, 1509.01388.

[8]  Dominique Derome,et al.  Hygroscopic Behavior of Paper and Books , 2007 .

[9]  M. Biot General Theory of Three‐Dimensional Consolidation , 1941 .

[10]  S. Tsai,et al.  Introduction to composite materials , 1980 .

[11]  O. Coussy Mechanics and Physics of Porous Solids: Coussy/Mechanics and Physics of Porous Solids , 2010 .

[12]  P. Perré,et al.  Microscopic tensile tests in the transverse plane of earlywood and latewood parts of spruce , 2000, Wood Science and Technology.

[13]  J. C. H. Affdl,et al.  The Halpin-Tsai Equations: A Review , 1976 .

[14]  O. Coussy Mechanics and Physics of Porous Solids , 2010 .

[15]  Misato Norimoto,et al.  Cell wall thickness and tangential Young's modulus in coniferous early wood , 2000, Journal of Wood Science.

[16]  Kent Persson,et al.  Micromechanical Modelling of Wood and Fibre Properties , 2000 .

[17]  P. Niemz,et al.  Distribution of structure and lignin within growth rings of Norway spruce , 2013, Wood Science and Technology.

[18]  Ruut Hannele Peuhkuri,et al.  Moisture and Bio-deterioration Risk of Building Materials and Structures , 2010 .

[19]  Nonlinear Poro-Elastic Model for Unsaturated Porous Solids , 2013 .

[20]  J. Boutelje The Relationship of Structure to Transverse Anisotropy in Wood with Reference to Shrinkage and Elasticity , 1962 .