Page 201 - Mechanics Analysis Composite Materials
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186                Mechanics and analysis of  composite materials

             where ATl =AT, =All, AT2 =Ar2 =A12,Ai2 =   =A22, AT4 = AT^ =A14, Ai4 =
             -AT4  =A24, A:4  =AT4 =A44, where A,,, (mn= 1I, 12,22, 14,24,44) are specified by
             Eqs. (4.72).  Substituting Eqs. (4.126) into  Eqs. (4.125) we arrive at the  following
             constitutive equations for an angle-ply layer:



                                                                              (4.127)



             The inverse form of these equations is

                                                                              (4.128)


             where



                                                                              (4.129)




             As follows from Eqs. (4.127) and (4.128), the layer under study is orthotropic.
               Now derive constitutive equations relating transverse shear stresses zxzand zy  and
             the corresponding shear strains yxz  and  yw.  Let the angle-ply layer be loaded by
             stress z,.   Then for all the plies, z:   = 7,;  = z,   and because the layer is orthotropic,
             yz = 7,;  = yu,  y-2 = y-;  = yjz = 0.  In  a  similar  way,  applying stress z,   we  have
             72 = T;  = z,,,   y-;  = y;  = y.y., 7:  = y,;  = 'yxr  = 0. Writing  two  last  constitutive
             equations of Eqs. (4.71) for these two cases we arrive at





             where stiffnesscoefficients A55  and A66  are specified by Eqs. (4.72).
               Dependencies of E, and G,,. on 4 plotted with the aid of Eqs. (4.129) are shown in
             Fig. 4.57 with solid lines. Theoretical curve for E,  is in very good agreement with
             experimental data  shown with circles (Lagace, 1985). For comparison, the  same
             moduli are presented for the +4 anisotropic layer considered in Section 4.3.1.  As
             can be seen, Ex (*4)  3 E,'.  To explain this effect, consider a uniaxial tension of both
             layers in the x-direction.While tension of +# ply and of -4  individual plies shown
             in  Fig.  4.58  is accompanied with shear strain, the system of these plies does not
             demonstrate shear under tension and, as a result, has higher stiffness. Working as
             plies  of  a  symmetric angle-ply layer individual anisotropic +4  and  -4  plies are
             loaded not only with normal stress a,  that is applied to the layer, but also with shear
             stress  zx-,,  that  restricts the  shear of  individual plies  (see  Fig. 4.58).  To  find  the
             reactive and balanced between the plies shear stress, we can use Eqs. (4.75). Taking
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