session 21 ic2011 niemz

43
"Cross Laminated Timber (CLT) panels - a new wood based material with high value added" Peter Niemz; ETH Zürich, Institute for Building Materials, Wood Physics, Switzerland [email protected]; www.ifb.ethz.ch/wood

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Page 1: Session 21 ic2011 niemz

"Cross Laminated Timber (CLT) panels - a new wood based material with high value added"Peter Niemz; ETH Zürich, Institute for Building Materials, Wood Physics, Switzerland

[email protected]; www.ifb.ethz.ch/wood

Page 2: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Outline

1. Introduction

2. Overview about works from the ETH, IfB/Wood Physics

1. Mechanical Properties2. Sorption, swelling, moisture induced stresses,

warping3. Thermal conductivity, diffusion4. Modeling

3. Examples for using from CLT2

Page 3: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

1. Introduction What is cross laminated timber? Wood based material based on solid wood

(boards) Boards or lamellas connected with adhesives,

nails, dowels, key and slots► Elements for the construction (format: 3.4m x

13.7m, up to 0.8m thickness), industrial prefabrication, Schilliger/CH, KLH/ Germany; Binder/Austria and other

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Page 4: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Solid wood wallsNägeli/CH, Thoma/A Soligno/I dowels (Nägeli, Thoma) key and slots nails (Hundegger)

high resistance during earthquake

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Page 5: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Plant for CLT, conected with dowels (Nägeli/CH)

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Page 6: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

prefabrication with CNC-machines

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Page 7: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Cross laminated timber, produced from glued cross laminated layers (3-11)start: around 1990 (G. Schickhofer/A, E. Gehri/CH)

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Lamellas in the middle layer glued or not glued together, gaps between lamellas (reduction from stresses)

Grading from surface lamellas (C14-C40), high quality surfaces (optical grading)

Possible loading: tension, compression, bending (beam, disc)

Page 8: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 8

Bending perpendicular

Board for a road bridge, max. load 40t (Fa. Schilliger Holz/CH)

F

Page 9: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 9

Bending parallel to the surface(higher tension perpendicular)

Roof construction (Fa. Schilliger Holz)

[email protected]

F

Page 10: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

costs

additional charge for timber construction(Nägeli/CH):

Timber frame construction: +5% Solid wood wall: +9-10%

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Page 11: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

2. Overview about works from the ETH, IfB/Wood Physics

2.1 Mechanical properties

Small samples, medium samples, boards, (scaling effect)

Calculation from mechanical properties (examples: plywood calculation according DIN 68765, FE-modeling, calculation as a laminated material (laminate theory)

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Page 12: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Board thickness: 30 mm; lamella ration: 1 = 10/10/10; 1,75 = 8/14/8; 3 = 6/18/6; small samples (Steiger und Niemz 2004)

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Bending strength = f(board structure)lamella ratio: thickness middle layer/thickness surface layer

In fibre direction

Perpendicular to the fibre

Page 13: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

failure by rolling shear (typical for small samples, not for entire board)

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Page 14: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Reduction from bending strength by slots

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bend

ing

stre

ngth

(N/m

m2 )

Without slots with slotsmiddle layer

in fibre dircetion

perpendicular to the fibre

Page 15: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Tests from boards and beams samples(scaling effect)

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PlattenversucheBalkenversuche

a al1

l

F/2 F/2

Test from beams:EN 789 (CEN 1995)

boards

beams

Page 16: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Test from entire boards4 single loads

2.5m x 2.5m x 0.07m), Empa/ETH

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Page 17: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Bending strength from beams and entire boards (Czaderski et al. 2007)

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Producer n min[N/mm2]

meanvalue

[N/mm2]

max[N/mm2]

median[N/mm2]

s[N/mm2]

x05[N/mm2]

beamsA 70 18.7 36.5 50.4 37.6 6.18 25.5

B 78 20.3 39.9 54.4 41.1 6.71 28.0

boardsA 12 35.1 50.7 61.4 50.0 8.20 35.1

B 12 49.6 59.8 68.6 59.5 5.86 48.0

B- better grading from wood

Page 18: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Examples for the calculation from MOE(Czaderski et al. 2007)

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parallel tot he grain perpendicular tot he grain

000, EEm 90090, EEm

plywood analogy (Steck 1988):

33

31

33

0 hhh

Gl. (4)

plywood analogy (Steck 1988):

33

31

90 hh

Gl. (5)

modified plywood analogy (Blass und Görlacher 2003):

33

31

0

9033

0

1

h

hEEh

Gl. (6)

modified plywood analogy (Blass und Görlacher 2003):

33

31

0

9033

0

90

90

1

h

hEEh

EE

Gl. (7)

Page 19: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Conclusions

Influence from fibre direction and board structure (layer ratio)

Using as beams, boards, discs, higher value for tensile strength perpendicular in relation to glue lam

Scaling effect

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Page 20: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

2.2 Sorption, swelling, moisture induced stresses, warping

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Page 21: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Sorption

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Lower EMC then solid wood

Internal stresses?Adehesives ?

Page 22: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Swelling and shrinkage

spruce: l = 0.01%/%, r =0.17%/%, t =0.3%/%

CLT:

in plane direction 0.016-0.025%/%

perpendicular: 0.3-0.5%/%

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Page 23: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) April 2011

Vertical profiles of EMC through the samples(Neutron Imaging, Sonderegger et al. 2010), 0%-20/85%

UF 1 C PUR no. of bond lines1

3

5

water73.75d 0.75d

Page 24: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Diffusion resistance factor

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020406080

100120140160180

Variant es

μ [-]

1 10 11 12 13

1 = lamellas glued,10 = not glued ,Distance between lamellas: 11 = 5mm, 12 = 10mm, 13 = 30mm

Dry Cup (20oC)0% - 65% RH.

Influence: µ encreased with no. of

layers Influence from adhesive Board structure (slots,

holes)

Page 25: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Thermal conductivity

Solid wood (spruce): (λspruce≈0,1W/mK)

Parameters: density, EMC, temperature

Solid wood panels (CLT): λCLT< λspruce, solid wood influence from growth rings influence no. of layers influence of holes

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Page 26: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Influence of board structure on thermal conductivity

CLT from spruce: (Bader et al. 2007)

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radial tangential without orientation

ther

mal

con

duct

ivity

(W/m

K)

Page 27: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Thermal conductivity from CLT:influence from the distance between lamellas

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0.080

0.085

0.090

0.095

0.100

0.105

0.110

0

λ [W

/m ּ◌K

]

10 11 12 13

Distance between lamellas in the middle layer: 10 = 0mm, 11 = 5mm, 12 = 10mm, 13 = 30mm

Page 28: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

2.3. Moisture induced stresses and swelling pressure

During strong drying cracks in the surface layer are possible

For panels in rooms with low air humidity EMC from around 8% necessary for surface layers

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Page 29: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Cracks in the surface layer during drying (surface layer too wet during production, compression strain needed in surface layer)

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Page 30: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Cracks in the surface layerconditions:production: (20oC/85%), drying (20oC/35%), tensile stresses

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Slots in the surface

without slots

Slots in the middle layer

before gluing:climatization under20oC/35% or20oC/65% not cracks detected(compression stresses)

Page 31: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Modeling of moisture transfer and moisture induced stresses-warping(PhD: Gereke 2009)

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el

Total strain:• elastic: Hooke law• Moisture induced: swelling• Mechano- sorptiv effect

future: viscoelastic+ plastic (PhD Hering 2011)

Page 32: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 32

FE-simulation moisture transfer (Gereke 2009) mit Abaqus

Page 33: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

FE-simulation warping (climatic conditions: 20/65%-20/100%, Gereke 2009)

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AR: growth ring angle0-tangential90-radial

LR: Lamella ratio

Pl

De

aa

LR

2

Page 34: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

3. Examples for using from CLT

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Page 35: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 35

Prefabricated house (Nägeli /CH)

Page 36: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

House produced with solid wood walls (Nägeli AG/CH, used wood: 300m3)

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Page 37: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

one family house (Pius Schuler/CH)

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Page 38: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 38

Monte Rosa cottage (Architects ETH)

Foto: Schilliger Foto: Purbond

Page 39: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 39

Bridge, produced with CLT and glue lam (Schilliger Holz/CH)

glue lam

CLT

Page 40: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected]) 40

Schoolhouse (Manchester), prefabricated in Switzerland (Schilliger Holz)

Page 41: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Timber tower (Germany, high: up to 160m)

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Page 42: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Thanks former PhD students Dr. Thomas Gereke, now UBC Vancouver

(modelling warping)

Dr. Walter Sonderegger (ETH)

(thermal conductivity, diffusion)

Dr. Matus Joscak (moisture transfer in wooden walls)

Stefan Hering (modelling stresses in bon lines)

and a lot of other peopels from mi group

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Page 43: Session 21 ic2011 niemz

Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; [email protected])

Thanks for your atention

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IfB, wood physics