Title: Anisotropic characteristics of wood dynamic viscoelastic properties
1Anisotropic characteristics of wood dynamic
viscoelastic properties
- Jianxiong Lu, Fucheng Bao and Jiali Jiang
- Key Laboratory of Wood Science and Technology of
State Forestry Administration - Research Institute of Wood Industry
- Chinese Academy of Forestry
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2Outline
2
Materials Methods
Results Discussions
4
Conclusions
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31. Introduction
Anisotropic of Chinese fir wood
Longitudinal Tracheids
(early- and latewood) Radial Tangential
Ray cells
- cell types
- cell arrangement
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4Aim scope
- Dynamic mechanical properties of wood in the
longitudinal, radial and tangential directions - Dynamic mechanical behaviors under tension and
flexural modes - The effects of freezing and heating treatments
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52. Materials Methods
2.1 Wood specimens
- Chinese fir(Cunninghamia lanceolata)heartwood
- The initial moisture content was about 82
- The average basic density was 0.27g/cm3
- Specimens were selected without knots and
defects
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6Dimensions of specimens
L sample
For the tension tests 35mm(L)6mm(R)1.5mm
(T)
For the single cantilever bending tests
35mm(L)12mm(R)2.5mm (T)
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7R sample
For the tension tests 35mm(R)6mm(L)1.5mm
(T)
For the single cantilever bending tests
35mm(R)12mm(L)2.5mm (T)
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8T sample
For the tension tests 35mm(T)6mm(L)1.5mm
(R)
For the single cantilever bending tests
35mm(T)12mm(L)2.5mm (R)
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92.2 Treatments
Freezing
- Pre- frost temperature - 29oC
- Condensation temperature - 49oC
- Sublimation vacuum degree 16.5Pa
- Treating time 25h
- Absolutely dried
Freeze-vacuum drying machine (FTS systems)
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10Heating
- Treating temperature 115oC
- Treating time 8h
- Absolutely dried
constant temperature drying machine (DX-400)
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112.3 Conditioning
Saturated solution of Magnesium Chloride (MgCl2)
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122.4 Measurements of the dynamic viscoelasticity
TA instruments DMA (Dynamic Mechanical
Analysis) 2980
- Temperature range-120 40oC
- Heating rate2oC/min
- Frequency1Hz
- Amplitude15um
- Tension flexural modes
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1317.65mm (L/R/T)
17.65mm(L/R/T)
2.5mm (T/T/R)
Preload force
0.01N
6mm(R/L/L)
Sinusoidally varying strain
Sinusoidally varying strain
1Hz 15um
1Hz 15um
Single cantilever bending
Tension
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142.5 E, E and Tand
Tand E/ E E storage modulus, an elastic
part, is a measure of the energy stored
elastically E loss modulus, a damping
component, is a measure of the energy lost as
heat Tand loss factor, a damping component, is
independent of a materials stiffness
E energy loss In internal motion
E elastic response
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153. Results Discussion
3.1 Anisotropy in storage modulus E
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16Temperature dependences of E for L, R and T
samples measured by tension mode
- The E decreased with the
- increase of temperature
- The E was much lower in
- the transverse than in the
- longitudinal direction
- the E in the radial was
- some 60 higher than that in
- tangential direction
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17Temperature dependences of E for L, R and T
samples measured by tension and single cantilever
bending modes
L sample
R sample
- The most significant difference was
- found for L sample
T sample
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183.2 Anisotropy in loss factor Tand
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19Temperature dependences of Tand for L, R and T
samples measured by tension mode
- a attributed to the glass
- transition of hemicellulose
ß
a
- ß due to the reorientation of
- methylol groups and adsorbed
- water molecules in amorphous
- of wood cell wall
- The intensity of transitions
- was highest for T sample
a
- Difference in loss peak
- temperatures
ß
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20Loss peak temperatures for L, R and T samples
measured by tension mode
Conflicted with synthetic composites where
the higher loss Peak temperatures were found in
the stiffer direction
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21Temperature dependences of Tand for L, R and T
samples measured by tension and single cantilever
bending modes
ß
a
L sample
a
ß
R sample
a
ß
- Difference in loss peak temperatures
T sample
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22Loss peak temperatures for L, R and T samples
measured by two mechanical modes
ß T gtR gt L
ß T gtR gt L
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233.3 Effect of freezing/heating treatments
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24L sample
- E heat gt virgin gt freeze
- Tand freeze gt virgin gt heat
- Difference in loss peak temperatures
Temperature dependences of E and Tand for three
kinds of L samples measured by tension mode
ß
a
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25R sample
- E heat gt virgin gt freeze
- Tand freeze gt virgin gt heat
- Difference in loss peak temperatures
Temperature dependences of E and Tand for three
kinds of R samples measured by tension mode
a
ß
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26T sample
- E heat gt virgin gt freeze
- Tand freeze gt virgin gt heat
- Difference in loss peak temperatures
Temperature dependences of E and Tand for three
kinds of T samples measured by tension mode
a
ß
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27Loss peak temperatures for virgin and treated
samples measured by tension mode
- Loss peak temperature Heating gt Virgin gt Freezing
- Due to their different equilibrium moisture
content - Heating (3.3) lt Virgin (4.8) lt Freezing
(5.1)
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284. Conclusions
1) The specimens oriented parallel to the grain
presented the highest storage modulus E, and the
E was much lower in the tangential direction
than in the radial direction
2) The L sample showed a lower ß -loss peak
temperature than that for the R and T samples,
which was in conflict with polymer
composites where the higher loss peak
temperatures were found in the stiffer direction
3) The rheological properties of wood showed a
dependence upon the mechanical modes used during
experiments. Tension mode presented higher
stiffness than the flexural mode
4) The dynamic viscoelastic behavior of wood was
affected by freezing or heating treatment.
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29Thank you for your attention
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