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Proceedings e report - Firenze University Press

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4. Results<br />

Young's modulus (10^4 Mpa)<br />

4<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

ELASTIC PROPERTIES OF MINUTE SAMPLES OF WOOD ALONG THE THREE MATERIAL DIRECTIONS<br />

34<br />

transverse plane<br />

Fig. 6 : Sampling in radial and tangential directions.<br />

(a)<br />

1<br />

0.4 0.45 0.5 0.55 0.6<br />

Density(g/cm3)<br />

T1<br />

T2<br />

T3<br />

T4<br />

T5<br />

N1<br />

N2<br />

N3<br />

N4<br />

O1<br />

O2<br />

Young's modulus (MPa)<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

(b)<br />

tangential<br />

direction<br />

radial direction<br />

0<br />

0.4 0.45 0.5 0.55 0.6<br />

Density (g/cm3)<br />

Fig. 8: Young's modulus of tension (T), normal (N) and opposite (O) wood in the longitudinal (a), radial and<br />

tangential (b) directions in relation with their density.<br />

Table 1 : Specific modulus of tension (T), opposite (O) and normal (N) poplar wood in radial (R), tangential (T)<br />

and longitudinal (L) directions.<br />

E (c) R ET EL Density E' (a) R E'T E'L<br />

T 1 143 416 34 300 0.55 2 078 756 62 364<br />

SD (b) 111 60 1 400 0.02<br />

O 1 170 478 15 500 0.47 2 489 1 017 32 979<br />

SD 269 109 2 000 0.05<br />

N 1 484 573 18 200 0.43 3 451 1 333 42 326<br />

SD 75 65 2 600 0.04<br />

(a) E’: Specific modulus (Mpa.kg -1 .m 3 )<br />

(b) SD: Standard deviation<br />

(c) E: Young’s modulus (MPa)<br />

Density (g/cm 3 )<br />

In the longitudinal direction, the variability of Young's modulus in the differences samples of each<br />

type of wood (tension, normal and opposite wood) is low compared to the transversal direction.<br />

Particularly, in the case of opposite wood, the standard deviation of the Young's modulus is rather<br />

high; the Young's modulus is variable despite the proximity of all samples to the same annual ring.<br />

This could be due to the fact that, as ring widths are very narrow in opposite wood, the sample can<br />

easily involve adjacent annual rings. For normal wood and tension wood, quite good values of<br />

standard deviation have to be noticed.<br />

In the longitudinal direction, the difference between tension wood and the group of normal and<br />

opposite wood is huge, E=35000MPa for tension wood and E=17000MPa for opposite and normal<br />

wood. On the contrary, the results in the transversal direction present low differences of Young’s<br />

E_rt<br />

E_ro<br />

E_rn<br />

E_tt<br />

E_to<br />

E_tn

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