• No results found

Three-dimensional orthotropic elastic-plastic-mechano-sorptive material model for simulation of wood behaviour

N/A
N/A
Protected

Academic year: 2022

Share "Three-dimensional orthotropic elastic-plastic-mechano-sorptive material model for simulation of wood behaviour"

Copied!
2
0
0

Loading.... (view fulltext now)

Full text

(1)

 

1

ECCM 2010

IV European Conference on Computational Mechanics Palais des Congrès, Paris, France, May 16-21, 2010

Three-Dimensional Orthotropic Elastic-Plastic-Mechano-Sorptive Material Model for Simulation of Wood Behaviour

Mats Ekevad

Luleå University of Technology, Div.Wood Science and Technology, Sweden, mats.ekevad@ltu.se

A material model for the macroscopic behaviour of wood is presented in this paper. Also results from three applications of the model are shown. The material model can handle dependence of moisture content (MC) and temperature on the elastic and non-elastic deformation of wood and wood structures. The non-elastic behaviour in the form of mechano-sorptive and plastic behaviour is of importance for wood drying applications but especially a variant of the plastic behaviour can also be used for wooden structures where there is slip possibilities between structural members. The material model is incorporated as user-supplied subroutines to the commercial FEM-code ABAQUS, [1].

Orthotropic linear elasticity and shrinkage is modelled with the elastic strain increment

M dT M du

F du dT

d F

d T u

e     

   00   . Here Fis the traditional orthotropic elastic flexibility matrix,

0and

0are the expansion coefficients for temperature and MC, respectively and the two last terms are due to the dependence of the elastic moduli on temperature and MC, respectively. For other notations and definitions, see [5]. Mechano-sorptive behaviour is modelled as an added mechano-sorptive strain increment d

msm

du in each of the radial, tangential and fibre direction. Plasticity is modelled as an added plastic strain increment

 

 

 f

d p where λ is a constant which is determined from the condition that df=0 during a plastic strain increment. Plasticity is only at hand when there is yield, i.e. when the yield function f=1. f in this orthotropic case is taken as a general polynomial expression which is similar to the well-known Tsai-Wu rupture surface. This yield function has the advantage that yield limits may be specified separately for each stress component and differently in compression and tension. It is also possible to use a variant with yield limits for stress components which depend on other stress components as is shown in the bridge example below. All material coefficients, elastic and non-elastic, may be specified as functions of temperature and MC.

The orthogonal directions may be specified locally for each point. If information of local fibre and growth ring direction is at hand (e.g. from computed tomography measurements [3]) these local directions may be used at every point. Otherwise a simplified calculation of local directions can be used.

The local and varying wood properties were modelled on a macroscopic scale in the three examples shown below. The variation between early-wood, late-wood, juvenile wood, heartwood and sapwood was not considered. Knots or other “defects” were not modelled. Material coefficients as a function of temperature and moisture content for Norway spruce (Picea abies) were used.

Twist of wooden boards was simulated with the elastic-plastic model, [4]. The drying was at first simulated with a diffusion model and a drying scheme from an ordinary drying kiln, [2]. Then the MC of the boards were used as input to a simulation of stresses and deformations with the elastic-plastic material model. The spiral grain angle of the boards was used as input to the model. The results

(2)

showed that it was possible to get realistic resulting twist values after drying compared to experimental values and also to simulate the influence of pretwist during drying of these boards.

Shrinkage of board cross sections was simulated with the elastic, the elastic-plastic and the elastic- mechano-sorptive model. The results show that there are small differences between results from different models for boards with the pith position outside of the cross section. However for boards with the pith position inside the cross section there are differences between the models. This is due to the fact that in the first case there are low stresses during shrinkage and in the second case there are high stresses. High stresses are relaxed during drying for the elastic-plastic and the elastic-mechano- sorptive models but are not for the elastic model.

A special variant of the elastic-plastic model (with yield stresses for two shear components that depend on one normal stress component) has recently been used to simulate slip between glue-lam beams in pre-stressed wooden road bridges. These bridges consist of a number of gluelam beams, side by side, that make up the bridge deck. The beams are held together with prestressed steel bars which give a contact pressure between the beams and thus the friction carries the load that is transferred between the beams. In this case it was interesting to simulate the onset of slip between the beams when the prestressing force was too low in relation to the traffic load. The individual beams of the bridge deck were not modelled individually; instead the bridge deck was modelled as a continuum and yield limits were set for two relevant shear stress components. The results show that this variant of the elastic-plastic model works well and is suited to this specific case since it possible to simulate frictional slip between the beams.

Shear stress for bridge deck with elastic-model.

No slip between beams.

Shear stress for bridge deck with elastic-plastic model. Slip between beams has reduced shear stresses.

References

[1] Anon. 2004. ABAQUS Users manual. ABAQUS, Inc., RI, USA. www.abaqus.com.

[2] Danvind, J. & Ekevad, M. (2006). Local water vapour diffusion coefficient when drying Norway spruce sapwood. J. Wood Science 52:195-201.

[3] Ekevad, M. (2004). Method to compute fiber directions from computed tomography images. J. Wood Science 50:41-46.

[4] Ekevad, M.; Salin, J.-G.; Grundberg, S.; Nyström, J. & Grönlund, A. (2006). Modelling of adequate pretwist for obtaining straight timber. Wood Material Science and Engineering 1:76-84.

[5] Ekevad, M. (2006). Modelling of Dynamic and Quasistatic events with Special Focus on Wood-Drying Distortions. Doctoral Thesis. Luleå University of Technology, Division of Wood Science and Technology.

2006:39, ISSN:1402-1544, ISRN:LTU-DT--06/39--SE.

2

References

Related documents

label for 1 h (optimum hybridisation time).. 8 activated biotin-MB-AuNP/miRNA-21 complex onto the transducing surface.

Democracies do not take up arms against each other. This axiom has attained the status of a mantra in the field of international relations. As previous research has shown, however,

The result from the implementation of the model by Oh et al [1] is given in the comparative performance maps below, where the estimated pressure ratio and efficiency is plotted as

Laminate in this work consists of an aluminium foil and a Low Density Polyethylene (LDPE) foil.. A fully annealed AA1200 aluminium foil and LDPE with the product name LD270

- 2 x Diesel Engines MTU 16 V 2000 TN90 (Low Speed Machinery, LSM) - 4 x Gas Turbines Honeywell TF50A (High Speed Machinery, HSM) - 2 x Main Reduction Gears (MRG) Cincinnati

Enligt Warden kan en strategisk entitet bestå av färre ringar än de fem beskrivna 7 , så även om resultatet blir att Al-Qaida inte kan sägas ha representation i alla fem ringar

Linköping University Medical Dissertations No... FACULTY OF MEDICINE AND

The dynamic simulation showed that the controller dosed precipitation chemical in the range between about 5-10 mg/l and that the effluent phosphate (S PO4 ) from