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Session 21 ic2011 niemz
1. "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
2. Outline
1. Introduction
2. Overview about works from the ETH, IfB/Wood
Physics
1. Mechanical Properties
2. Sorption, swelling, moisture induced stresses,
warping
3. Thermal conductivity, diffusion
4. Modeling
3. Examples for using from CLT
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 2
3. 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 3
4. Solid wood walls
Nägeli/CH, Thoma/A Soligno/I
dowels (Nägeli, Thoma) key and slots
nails (Hundegger)
high resistance during earthquake
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 4
5. Plant for CLT, conected with dowels
(Nägeli/CH)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 5
7. Cross laminated timber, produced from
glued cross laminated layers (3-11)
start: around 1990 (G. Schickhofer/A, E. Gehri/CH)
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) 7
8. Board for a road bridge, max. load 40t
(Fa. Schilliger Holz/CH)
Bending
perpendicular
F
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 8
9. Roof construction (Fa. Schilliger Holz)
Bending parallel to
the surface
(higher tension
perpendicular) F
info@schilliger.ch
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 9
10. costs
additional charge for timber construction
(Nägeli/CH):
Timber frame construction: +5%
Solid wood wall: +9-10%
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 10
11. 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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 11
12. Bending strength = f(board structure)
lamella ratio: thickness middle layer/thickness surface layer
In fibre direction
Perpendicular to the fibre
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)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 12
13. failure by rolling shear (typical for small
samples, not for entire board)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 13
14. Reduction from bending strength by slots
bending strength (N/mm2)
in fibre dircetion
perpendicular to the fibre
Without slots with slots
middle layer
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 14
15. Tests from boards and beams samples
(scaling effect)
boards
su ch e
Ba
lke en ver Test from beams:
t
nve beams P lat EN 789 (CEN 1995)
rsu a l1 a
che F/2 F/2
l
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 15
16. Test from entire boards
4 single loads
2.5m x 2.5m x 0.07m), Empa/ETH
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 16
17. Bending strength from beams and entire
boards (Czaderski et al. 2007)
Producer n min mean max median s x05
[N/mm2] value [N/mm2] [N/mm2] [N/mm2] [N/mm2]
[N/mm2]
beams
A 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
boards
A 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) 17
18. Examples for the calculation from MOE
(Czaderski et al. 2007)
parallel tot he grain perpendicular tot he grain
Em ,0 E0 0 E m ,90 E0 90
plywood analogy (Steck 1988): plywood analogy (Steck 1988):
h h
3 3 3
h
0 3 3 1 Gl. (4) 90 13 Gl. (5)
h3 h3
modified plywood analogy modified plywood analogy (Blass
(Blass und Görlacher 2003): und Görlacher 2003):
E 3 E90 3 E 3
h3 1 90 h1 h3 1 90 h1
3
E0 E0
0 Gl. (6) 90
E0 Gl. (7)
3 3
h3 h3
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 18
19. 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 19
20. 2.2 Sorption, swelling, moisture induced
stresses, warping
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 20
21. Sorption
Lower EMC
then solid wood
Internal stresses?
Adehesives ?
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 21
22. 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%/%
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 22
23. Vertical profiles of EMC through the samples
(Neutron Imaging, Sonderegger et al. 2010), 0%-20/85%
UF 1 C PUR no. of bond
73.75d 0.75d
water lines
1
3
5
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)
April 2011
24. Diffusion resistance factor
180 Dry Cup (20oC)
160 0% - 65% RH.
140
120 Influence:
100 µ encreased with no. of
μ [-]
80 layers
60 Influence from adhesive
Board structure (slots,
40
holes)
20
0
Variant es
1 10 11 12 13
1 = lamellas glued,10 = not glued ,
Distance between lamellas: 11 = 5mm, 12 = 10mm, 13 = 30mm
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 24
25. 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 25
26. Influence of board structure on thermal
conductivity
CLT from spruce: (Bader et al. 2007)
radial tangential without orientation
thermal conductivity (W/mK)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 26
27. Thermal conductivity from CLT:
influence from the distance between lamellas
0.110
0.105
0.100
ּ K]
λ [W/m◌
0.095
0.090
0.085
0.080
10 11 0 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) 27
28. 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 28
29. Cracks in the surface layer during drying
(surface layer too wet during production, compression
strain needed in surface layer)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 29
30. Cracks in the surface layer
conditions:
production: (20oC/85%), drying (20oC/35%), tensile stresses
Slots in the surface
before gluing:
climatization under
20oC/35% or
20oC/65%
without slots
not cracks detected
(compression stresses)
Slots in the middle layer
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 30
31. Modeling of moisture transfer and
moisture induced stresses-warping
(PhD: Gereke 2009)
Total strain:
• elastic: Hooke law
• Moisture induced: swelling
• Mechano- sorptiv effect
el
future: viscoelastic+ plastic (PhD Hering 2011)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 31
32. FE-simulation moisture transfer
(Gereke 2009) mit Abaqus
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 32
33. FE-simulation warping
(climatic conditions: 20/65%-20/100%, Gereke 2009)
AR: growth ring angle
0-tangential
90-radial
LR: Lamella ratio
2 a De
LR
a Pl
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 33
34. 3. Examples for using from CLT
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 34
35. Prefabricated house (Nägeli /CH)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 35
36. House produced with solid wood walls
(Nägeli AG/CH, used wood: 300m3)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 36
37. one family house (Pius Schuler/CH)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 37
38. Monte Rosa cottage (Architects ETH)
Foto: Schilliger Foto: Purbond
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 38
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) 39
40. Schoolhouse (Manchester), prefabricated
in Switzerland (Schilliger Holz)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 40
41. Timber tower (Germany, high: up to 160m)
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 41
42. 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
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 42
43. Thanks for your atention
IfB, wood physics
Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 43