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Heat affects
Hygroscopicity
Shrinkage & swelling
Mechanical properties
Acoustical properties
Electrical properties
Dimensional changes
Changes very small compared to shrinkage & swelling due to MC changes
No practical importance because temp changes normally within narrow limits & MC produces higher change.
Thermal expansion coefficient
Calculated for ovendry wood
d = (l2 - l1) / l1
Expansion coefficient a = d / l1*ΔT (given)
Elongation with 1C increase
smallest in axial & largest in tangential direction
Other dimensional
In plywood thermal expansion is different for each layer in same direction; washboard effect
a is largest with change in density in tangential direction. Radial lower. Axial very low with small change.
Thermal conductivity κ
Measure for amount of heat (kcal) flowing during time t (h) through a body with length t (m) & surface area A (m2) at temp T (K).
kcal*m/(h*m*K) → W/(m*K)
Inverse to thermal insulation capacity
Good insulation quality because of porous structure
Thermal conductivity dependencies
Wood structure
Density
MC
Temp
Extractives
Defects
κ with structure
κ higher in axial direction (about twice)
κ hardly varies between radial & tangential directions
axial: 0.191-0.284, radial: 0.104 - 0.151, tangential: 0.090 - 0.14
Higher axial value due to fibrous morphology & axial orientation of wood cells
Deviations of fibrils in vertical orientation reduce axial conductivity
Radial conductivity about 5-10% higher than tangential because of wood rays
Higher tangential conductivity in species with pronounced density difference between early/latewood
Ratio of axial:tangential conductivity depends on angle of microfibrils in S2 wall
large angle decreases ratio
Thermal conductivity linearity
TC varies linearly with density, MC, temp.
Density and MC & TC formula
κ = 0.177R12 + 0.0205
R12 is density at 12% MC
κ = 0.01864 + r0(0.1941 + 0.004604*MC)
Extractives & TC
High extractive content means higher conductivity
Insulation properties
Wood is good thermal insulator
Light & dry wood better
Low temp better
Specific heat
Amount of energy needed to increase temp of a mass by 1C
J/ g*C
High specific heat with low thermal conductivity makes wood suitable for handles, matches, ect.
Not affected by species, density, but increases with temp & MC
Combustion
Wood burns at high temp; suitable for energy/heat production, limitation as building material
Result is chemical decomposition
Flammable gases produced
Process:
Moisture evaporates (up to 100C)
Volatile substances evaporate (95 – 150oC)
Carbonisation of the surface and slow exit of flammable gases (150 - 200oC)
Increased exit of flammable gases, ignition and glow (200 - 370oC)
Ignition of flammable gases, formation of glowing charcoal (370 - 500oC)
Flammability dependencies & stages
Depends on species, MC, temp, dimensions, type of structure.
Species;
extractives (mainly resin) increases flam
long, open passages (vessels) more flam
SW tracheids decrease flam, because short & closed ends
MC retards ignition & decreases flam
Temp increase increases flam
Stages
200 - 275oC: a external flame (spark) is needed to ignite the wood and maintain the flame.
260 - 290oC: Wood needs to be ignited external but the flame remains.
330 - 520oC: Spontaneous ignition.
Flammability & char
Small pieces burn easier & ignite at lower temp
In large structures only outside layer is burnt & core maintains strength
Carbonised layer has lower thermal conductivity & high specific heat. Acts as thermal insulator. Burning of core delayed.
Flammability reduced by impregnation
Heating value H
Amount of energy produced from burning 1kg (1g) of wood
kcal/kg or cal/g OR MJ/kg or J/g
Average max heating value of ovendry wood: 4500 cal/g
1kcal = 4.1868 kJ
MC & heating value
H of air dry wood about 15% lower than of ovendry wood
H of moist wood estimated by; H = H0*(1-u) - 2.45*u, u is MC in %
Extractives & heating value
SW generally have higher H
Chemical composition & heating value
Lignin has higher H value than cellulose
Lignin: 6100 kcal/kg
Cellulose: 4200 kcal/kg
Density and particle size & heating value
Increases with density
Decreases with particle size, but huge jump from smallest particle size to next range