Post on 10-Jul-2015
"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
niemzp@ethz.ch; www.ifb.ethz.ch/wood
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Solid wood wallsNägeli/CH, Thoma/A Soligno/I dowels (Nägeli, Thoma) key and slots nails (Hundegger)
high resistance during earthquake
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Plant for CLT, conected with dowels (Nägeli/CH)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
prefabrication with CNC-machines
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 8
Bending perpendicular
Board for a road bridge, max. load 40t (Fa. Schilliger Holz/CH)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 9
Bending parallel to the surface(higher tension perpendicular)
Roof construction (Fa. Schilliger Holz)
info@schilliger.ch
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
costs
additional charge for timber construction(Nägeli/CH):
Timber frame construction: +5% Solid wood wall: +9-10%
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
failure by rolling shear (typical for small samples, not for entire board)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Test from entire boards4 single loads
2.5m x 2.5m x 0.07m), Empa/ETH
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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):
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31
33
0 hhh
Gl. (4)
plywood analogy (Steck 1988):
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31
90 hh
Gl. (5)
modified plywood analogy (Blass und Görlacher 2003):
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31
0
9033
0
1
h
hEEh
Gl. (6)
modified plywood analogy (Blass und Görlacher 2003):
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31
0
9033
0
90
90
1
h
hEEh
EE
Gl. (7)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
2.2 Sorption, swelling, moisture induced stresses, warping
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Sorption
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Lower EMC then solid wood
Internal stresses?Adehesives ?
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Cracks in the surface layer during drying (surface layer too wet during production, compression strain needed in surface layer)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 32
FE-simulation moisture transfer (Gereke 2009) mit Abaqus
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
3. Examples for using from CLT
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 35
Prefabricated house (Nägeli /CH)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
House produced with solid wood walls (Nägeli AG/CH, used wood: 300m3)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
one family house (Pius Schuler/CH)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 38
Monte Rosa cottage (Architects ETH)
Foto: Schilliger Foto: Purbond
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 39
Bridge, produced with CLT and glue lam (Schilliger Holz/CH)
glue lam
CLT
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 40
Schoolhouse (Manchester), prefabricated in Switzerland (Schilliger Holz)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Timber tower (Germany, high: up to 160m)
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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
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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Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
Thanks for your atention
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IfB, wood physics