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effect of contiguity on shear elastic modulus of fibre reinforced ...

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18 Raluca Hohan, Liliana Bejan and Nicolae Ţăranu<br />

Experimental results indicate the adequacy <str<strong>on</strong>g>of</str<strong>on</strong>g> Halpin-Tsai eqs. to<br />

predict the <strong>shear</strong> <strong>modulus</strong> for practical requirements. Fig. 9 presents the<br />

influence <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>c<strong>on</strong>tiguity</str<strong>on</strong>g>, <strong>on</strong> <strong>shear</strong> <strong>modulus</strong>, versus extreme values <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>c<strong>on</strong>tiguity</str<strong>on</strong>g><br />

(C = 0 and C = 1). As it can be noticed in Fig. 9 the Halpin-Tsai numerical<br />

results coincide with those based <strong>on</strong> the <str<strong>on</strong>g>c<strong>on</strong>tiguity</str<strong>on</strong>g> factor (eq. (7)) when C = 0.<br />

Fig. 9 – Shear <strong>modulus</strong> predicted through Halpin-Tsai equati<strong>on</strong>s<br />

versus influence <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>c<strong>on</strong>tiguity</str<strong>on</strong>g> factor.<br />

4.2. The Composite Cylinder Assemblage (CCA) model<br />

This model enables the exact analytical evaluati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the <str<strong>on</strong>g>effect</str<strong>on</strong>g>ive<br />

<strong>elastic</strong> moduli (J<strong>on</strong>es, 1999). The model c<strong>on</strong>sists <str<strong>on</strong>g>of</str<strong>on</strong>g> an assemblage <str<strong>on</strong>g>of</str<strong>on</strong>g> composite<br />

cylinders (Fig. 10 a) each made <str<strong>on</strong>g>of</str<strong>on</strong>g> a circular <strong>fibre</strong> core and a c<strong>on</strong>centric matrix<br />

shell (Zweben, 1995).<br />

In each cylinder the <strong>fibre</strong> volume fracti<strong>on</strong> is kept c<strong>on</strong>stant (also<br />

meaning that the ratio r 2 /R 2 is the same); each composite cylinder behaves as an<br />

equivalent homogeneous cylinder. The volume <str<strong>on</strong>g>of</str<strong>on</strong>g> the material is progressively<br />

filled out with composite cylinders with different radii. C<strong>on</strong>sequently, the<br />

properties <str<strong>on</strong>g>of</str<strong>on</strong>g> the assemblage approach the properties <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>on</strong>e composite cylinder,<br />

The following formula corresp<strong>on</strong>ds to CCA model:<br />

GV + G (1 + V)<br />

.<br />

(1 )<br />

m m f f<br />

G12 = Gm GV f m + Gm + Vf<br />

(12)

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