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




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   5
prefabrication with CNC-machines




Portland 6-2011    Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   6
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
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
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
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
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
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
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
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
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
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
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
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
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
2.2 Sorption, swelling, moisture induced
    stresses, warping




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   20
Sorption


                                                                                                 Lower EMC
                                                                                                   then solid wood
                                                                                                 Internal stresses?
                                                                                                 Adehesives ?




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)                  21
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
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
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
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
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
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
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
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
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
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
FE-simulation moisture transfer
              (Gereke 2009) mit Abaqus




Portland 6-2011        Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   32
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
3. Examples for using from CLT




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   34
Prefabricated house (Nägeli /CH)




Portland 6-2011         Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   35
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
one family house (Pius Schuler/CH)




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   37
Monte Rosa cottage (Architects ETH)




                  Foto: Schilliger                   Foto: Purbond
Portland 6-2011           Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   38
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
Schoolhouse (Manchester), prefabricated
in Switzerland (Schilliger Holz)




Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   40
Timber tower (Germany, high: up to 160m)




 Portland 6-2011   Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   41
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
Thanks for your atention




                                                                  IfB, wood physics




Portland 6-2011     Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch)   43

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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
  • 6. prefabrication with CNC-machines Portland 6-2011 Peter Niemz (Institute for Building Materials, Wood Physics; niemzp@ethz.ch) 6
  • 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