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ETH Zurich Institute for Building Materials (IfB), Wood Physics Group www.ifb.ethz.ch ; [email protected] Solid wood panels – a new wood based material with high value added Peter Niemz

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Page 1: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

ETH Zurich

Institute for Building Materials (IfB), Wood Physics Group

www.ifb.ethz.ch; [email protected]

Solid wood panels – a new wood based material with high value added Peter Niemz

Page 2: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

211/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Outline

1. Introduction2. Modelling of Properties

2.1 Mechanical Properties• MOE• MOR

Experimental Tests2.2Physical Properties • Sorption• Swelling• Warping• Internal stresses

3. Conclusions

Page 3: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

311/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

1. Introduction

x 1

x 2

x 3

3

32

31

13

12

1

23

2

21

(z)

(x)

(y)

What is a solid wood panel?3 or 5 layer cross laminated board (system from plywood)

Board: up to 0.5m (thickness)x3m x15m

Page 4: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

411/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

What is a solid wood panel?• Solid wood panels represent a new multilayer material based on boards, which are glued together crosswise, in most cases spruce wood is used

• Used more and more in timber constructions providing a high value added

• The utilisation of this kind of panel gains in importance in the Swiss, German and Austrian building industry

• It is possible to vary the properties of the panels through panel configuration

Page 5: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

511/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Utilisation of solid wood panels as building material

Page 6: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

611/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Industrial prefabrication (Schilliger AG, Switzerland)

Page 7: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

711/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Roof constructions with solid wood panels

Page 8: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

811/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

House built with solid wood panels

Page 9: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

911/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

2. Modelling of Properties

2.1 Mechanical Properties

The load direction

surface layer parallel

surface layer perpendicular

(II) () MOE, pure bending

Eb(II) (N/mm2) Eb()

(N/mm2)

Shearing strength (rolling shear)

13(rol. shear) (N/mm2) 231)

(N/mm2)

Shear module

G13 (N/mm2) G231)

(N/mm2)

Bending perpendicular to the surface

Page 10: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1011/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

rolling shear (r-t) in middle layer

Page 11: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1111/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

a) Modulus of elasticity, if L/h>35 Navier-Bernoulli pure bending

33)2(

13

3)1(

1,22

1

v

v

v

vboardb

L

LE

L

LEE

E1 (1): Elastic module 1 (surface layer) with load in direction 1

E1 (2): Elastic module of layer 2 (middle layer) with load in direction 1

Eb,ges: Elastic module of cross section

Lv: Relation of lamellas-thicknesses; Lv= h (2)/h (1)

h (1): Thickness of the surface layerh (2): Thickness of the middle layer

(N/mm2)

MOE (Young’s modulus)MOE (Young’s modulus)

For surface layer orientation parallel to the longitudinal axis:

E1 (1) = EL = 11000 N/mm2; v = 15%E1 (2) = ER/T = 450 N/mm2

For surface layer orientation perpendicular to the longitudinal axis:E2 (1) = ER/T = 450 N/mm2

E2 (2) = EL= 11000 N/mm2; v = 20% (lower quality in the middle layer)

Page 12: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1211/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

b) Modulus of elasticity, if L/h<35 (parallel)

c

EE b

bx

1

2

2)2(

13

)1(13

Re2

)2(1

)1(13

3)1(

1

21224/

2

v

v

v

Su

v

vL

L

LG

L

GhL

EEL

LEK

c

(N/mm2)

Eb-E by pure bending

Exb _ E diminished by shearing

E = f (Bending + shearing)

Page 13: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1311/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

calculated influence of the lamella ratio on the MOE

(pure bending)

0

2000

4000

6000

8000

10000

12000

0.0 1.0 2.0 3.0 4.0 5.0thickness middle/surface layer

MO

E

Eb,

boar

d (N

/mm

2 )

Eb,équi(II)

Eb,équi(per)

cv=15%: surface layer parallel, cv=±20% surface layer perpendicular

Page 14: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1411/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Tests on an entire board, supported at all edges

(together with the Empa/Dübendorf, Dep. of structural Engineering)

Page 15: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1511/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Overview of panel tests

Lod Board structure No

boards

A 4 loads

1 10/50/10 mm 6

A 4 loads

2 25/20/25 mm 6

B 1 load, centric

1 10/50/10 mm 6

C 1 load, excentric

1 10/50/10 mm 6

Overview of panel tests

Page 16: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1611/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Failure of an entire board, not failure by rolling shear

Page 17: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1711/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Producer n Min[N/mm2]

Mean[N/mm2]

Max[N/mm2]

Median[N/mm2]

s[N/mm2]

x05

[N/mm2]

v[%]

Beam tests

A 70 18.7 36.5 50.4 37.6 6.18 25.5 16.9

B 78 20.3 39.9 54.4 41.1 6.71 28.0 16.8

tests at entire board

A 12 35.1 50.7 61.4 50.0 8.20 35.1 16.2

B 12 49.6 59.8 68.6 59.5 5.86 48.0 9.80

Failure stresses determined from beam and panel tests

• maximal strain tested in tensile zone from the board: 2-3%, • solid wood 1%

publication „Holz als Roh und Werkstoff“ (2007), test of different models

Page 18: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1811/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

2.2 Physical Properties

a) Equilibrium moisture content (calculated with Hailwood Horrobin)

Page 19: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

1911/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

sample m2/g UFS UP UM

MHP-3-27pa 265 20.49 13.01 7.47

MHP-3-27pe 249 21.06 14.03 7.04

MHP-3-30pa 269 20.86 13.27 7.60

MHP-3-30pe 235 22.43 15.79 6.64

Surface layer: Pa: parallel; Pe: perpendicular

Calculated parameters for sorption Calculated parameters for sorption (Hailwood Horrobin)(Hailwood Horrobin)

=specific surface, up= polymolecular water, um= monomolecular water

Page 20: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2011/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

b) Swelling (board thickness 60mm)

• thickness 0,3-0,5%/%

• length 0,045 %/%, (20/20/20)

0,016 %/%, (10/40/10) 0,021%/%, (12/12/12/12/12)

Influence from board structure (relation surface/middle layer)

Page 21: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2111/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

c) Diffusion resistence

• Adhesive types tested : PVA, UF, PUR (2 types), Resorcin• 3 and 5 layer solid wood panels with different lamella ratios

0% 12%0%

0% 0%

12%

12%12%

Trockenm ittelS ilikagel

K lim a aussen:20°C / 65% rF

K lim a innen :20°C / 0% rF

Theore tische H olz feuchtigke it

V ersuchsbeg inn V ersuchsende

Page 22: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2211/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

y = 20.913x - 4.3976

R2 = 0.883

y = 34.993x + 74.066

R2 = 0.8972

-10.0

40.0

90.0

140.0

190.0

240.0

290.0

340.0

0 1 2 3 4 5 6

no. of gluelines

dif

us

ion

re

sis

ten

ce

μ [

-]

wet cup (100%/65%)

dry cup (0%-65%rH)

Influence of the number of gluelines (for 1K PUR)

Page 23: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2311/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

• The water vapour diffusion resistance is strongly related to the number of glue layers per panel thickness

• No influence on the water vapour diffusion resistance by the utilisation of different types of adhesives was found

• The diffusion resistance decreased while the EMC increased

Results diffusion resistance

Page 24: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2411/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

d) Internal stresses

0 10 20 30 40 50 60

Dicke (mm)

0

1

2

3

4

5

6

7

8

9

10

Feu

chte

geh

alt

(Vo

l%)

0

2

4

6

8

10

12

14

16

18

20

22

Masse%

77

177177

0 0

2828

Zeit in Tagen

Zeitlicher Verlauf der gemessenen HolzfeuchtewerteMassivholzplatte, Lagerung im Konstantklima

Moisture distribution in wood panels 2oC/90% RH

Page 25: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2511/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Result:Internal cracks or warping from boards

different EMC during production and use

different EMC at both sides from the board

Page 26: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2611/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Hindered shrinking of a 3-layer solid wood panel

Page 27: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2711/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Modelling of warping and internal stresses in glued wood

a) example: 3-layer parquet element, oak-spruce-spruce

veneer; thickness: 14mm (3/8/3mm), diploma thesis

b) 2006 we started a PHD about internal stresses

in solid wood panels

Page 28: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2811/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Moisture transfer Transfer model, Diffusion 1D

2

31

D

D

e ff.oak

e ff.p ine

u a ir = u top surface

u a ir bottom surface= u

0.1m m U F res in

0.1m m U F res in

Model in ABAQUS

x

uuD

xt

uW )(

u in itia l u final

uzh

h

oak

pine

100

.0

.1.2

plate

plateuplateuplate m

mmu

)

1001()

1001( 2

.02

.0.pine

pinepineoak

oakoakplateu

ubh

ubhm

pineoak

pineoakpine

pineoak

oak

ABAQUS hhn

hhnu

hu

hn

u

100

~1

100

~1

Iteration-method

simplification- Deff constant- without glueline- without surface material

Calculation of the influence from glue lines is possible, but material parameters are necessary

Page 29: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

2911/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Model A: Warping from parquetABAQUS FE Model

2

3

1 u2=0

u1= 0A (10 /14 .2 /13)

B (94 /14 .2 /13 )

u3=0

v B

A

M ois tu re exchangelim ited to the top su rface

94

Model- 3D brick Elements- 20 Points, quadr.

interpolation- mash size 2mm

Beam theory

L 1L 2L 3L e k v

N

N 2

N 3

L e kv

M

yc

1

(a) (b)

12

3

ekv

u i

ekv

M 1

M 2

M 3

beAx

2min e

x

Page 30: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3011/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Beech

Oak

Ash

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Beech

Oak

Ash

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Beech

Oak

Ash

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Beech

Oak

Ash

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Beech SL 3.6mm

Oak SL 3.6mm

Ash SL 3.6mm

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Angle = 30degAngle = 45 degAngle = 0 degAngle = 90 deg

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Angle = 30degAngle = 45 degAngle = 0 degAngle = 90 deg

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Angle = 30degAngle = 45 degAngle = 90 degAngle = 0 deg

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Angle = 30degAngle = 45 degAngle = 90 degAngle = 0 deg

Influence of the grain angle in the surface layer

Page 31: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3111/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Surface layer 2.6mm

Surface layer 3.6mm

Surface layer 4.8mm

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Surface layer 4.8mm

Surface layer 3.6mm

Surface layer 2.6mm

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Surface layer 2.6mm

Surface layer 3.6mm

Surface layer 4.8mm

0 20 40 60 80 100 1200

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

Time [days]

Cu

pp

ing

v [m

m]

Surface layer 4.8mm

Surface layer 3.6mm

Surface layer 2.6mm

Influence of the layer thicknesses

Page 32: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3211/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Model B: Stresses in the glue line and gap opening

Page 33: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3311/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Stress analysis (for parquet; investigations on solid wood panels are ongoing)

Longtime study cut A-A

-15 -10 -5 0 5 10 15 20 25-1

-0.5

0

0.5

1

1.5

2

Horizontal distance to middle gap [mm]

Ver

tica

l stre

sses

S2

2 [M

Pa]

L= 0,

R,T= 0

L= 0.1,

R,T= 0.8

L= 0.3,

R,T = 1.6

L= 1.5,

R,T= 7

A ABD

B

E CC

-15 -10 -5 0 5 10 15 20 25-2

-1.5

-1

-0.5

0

0.5

1

1.5

2

Horizontal distance to middle gap [mm]

Sh

ea

r st

ress

es

S1

2 [M

Pa

]

L= 0,

R,T= 0

L= 0.1,

R,T= 0.8

L= 0.3,

R,T = 1.6

L= 1.5,

R,T= 7

Periodic loading increases the creeping , effect delamination can occur after several summer – winter cycles.

Page 34: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3411/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

ongoing works

Page 35: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3511/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

On-line testing free swelling hindered swelling

Testing of internal stresses

Page 36: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3611/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Results (spruce)

Swelling pressure

0 5 10 150

0.2

0.4

0.6

0.8

1

1.2

1.4

time [d]

pres

sure

pQ [k

N/m

m²]

Fichte (tangential)

Fichte (radial)

Fichte (longitudinal)

MDF (Plattenebene)

Dreischichtplatte

Page 37: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3711/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

Results (spruce)

Free swelling

0 5 10 150

0.5

1

1.5

2

2.5

time [d]

swel

ling

α [%

/%]

Fichte (tangential)Fichte (radial)Fichte (longitudinal)MDF (Plattenebene)DSP (stehende Jahrringe)DSP (liegende Jahrringe)

00

0.05

0.1

0.15

0.2

0.25

0.3

0.35

Page 38: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3811/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

3. Conclusions

Solid wood panels have a very high value added

(producer mostly saw mills)

Properties can be calculated

Scientifically interesting field of work

Page 39: ETH Zurich Institute for Building Materials (IfB), Wood Physics Group ; niemzp@ethz.ch © ETH Zürich Solid wood panels – a

3911/2006 Peter Niemz, IfB Wood Physics Group, [email protected]

IfB, Wood Physics

Any Questions?