An abstract of the thesis of



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Bog'liq
Edward Le PhD Dissertation

1/D
t
(mm/MPa)
MO
E (MPa
)
1% Glue
25% Glue
PF
10% 0%
30%
20%
100% Glue
Figure 3.11. Simulation results of MOE versus 1/D
t
at different levels of compaction for 
OSL. 
3.6.3 Plywood – Numerical Modeling of OSB with No Gaps 
If gaps are eliminated from the OSB simulations, the structure has continuous 
layers and is essentially a 3-layer plywood. When plywood is compressed, the layers 
densify, but there is no undulation (see Figure 3.12). These simulations with no gaps can 
assess the role of strand undulation in glue-line effects.


60 
a)
0% compaction 
b)
10% compaction 
c)
20% compaction 
d)
30% compaction 
e)
40% compaction 
f)
50% compaction 
Figure 3.12. Sample simulation of OSB with no gaps at different levels of compaction. 


61 
4500
5000
5500
6000
6500
7000
7500
0.00
0.01
0.02
0.03
0.04
0.05
1/D
t
(mm/MPa)
MO
E
 (
MP
a
)
OSB
Plywood
Figure 3.13. Simulated MOE versus 1/D
t
for plywood and OSB at 30% 
compaction 
Figure 3.13 shows results of axial MOE versus 1/D
t
at 30% compaction for OSB 
and plywood. The plywood is just a special case of OSB with no gaps. In Figure 3.13 
OSB results depended on the interface but plywood did not. As 1/D
t
increased, plywood 
gave a straight horizontal line or was nearly independent of D
t
. Furthermore, the MOE in 
tension for plywood was much higher than for OSB. Therefore, as the strand length 
increases and/or the gap spacing decreases, the mechanical properties of OSB will 
increase and approach the mechanical properties of the analogous plywood. In Figure 
3.13, all data were obtained from an average of at least five runs. The error bars on the 
OSB curve show the standard deviations of these results. There are no error bar on 
plywood because only one structure could be analyzed (i.e., no way to repeat for different 
structures).


62 
Similarly, if gaps are removed for OSL simulations, the structure is essentially 
LVL (laminated veneer lumber) and strand undulation stops. Figure 3.14 shows results of 
axial MOE versus 1/D
t
at 10% compaction for OSL and LVL in tension. The mechanical 
properties of the LVL are higher than OSL. The error bars in Figure 3.14 on the OSL 
curve represents the standard deviation from average of five runs. As 1/D
t
increased, 
LVL gave a straight horizontal line or was independent of D
t
. Therefore, as the strand 
length increases and/or the gap spacing decreases, mechanical properties of OSL panel 
will approach the mechanical properties of LVL. In other words, they will improve and 
become less affected by D
t
.
5500
6000
6500
7000
7500
8000
8500
9000
9500
10000
10500
0.000
0.020
0.040
0.060
0.080
0.100

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