Page 330 - Mechanics Analysis Composite Materials
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Chapter 7.  Environmental, special loading. and manufacturing ~@c.cts   315

                M:,  =Jif'- d;:)= 1840 x  10-'AT  GPa mm'/"C,
                M?;__  = 5100 x   AT GPa  mm'/"C  .

            Thus,  the  thermal  terms  entering costitutive  equations  of  thermoplasticity,  Eqs.
            (7.23),  are  specified.  Apply  the  obtained  results  to  determine  the  apparent
            coefficients of thermal  expansion  for  the space telescope section  under  study (see
            Fig. 7.3). We can assume that under uniform heating the curvatures do not change
            in the middle part of the cylinder so that  K,T  = 0 and K,T  = 0. Because there are no
            external loads, free body diagram allows us to conclude that N, = 0 and N, = 0. As
            a result, the first two equations of Eqs. (7.23) for the structure under study become:

                               N:,
                             =
                BIIe:.,  +BI~E~~
                B',  E!.,  + ~22.~:~= N&-- .
            Solving these equations for thermal strains and taking into account Eqs. (7.20) we
            get




                     1
                                             .
                Fo,IT - -(BIIN,T,-B12N;I;)= CI~.AT
                   -
                     B
            where B = BIIB~~B!?. For the laminate under study, calculation yields
                           -
               CI,  = -0.94  x  10.'  1/"C,   CI,.  = 14.7 x  l/"C .

            Return  to  Eqs. (7.13)  and  (7.20)  based  on  the  assumption  that  coefficients
            of  thermal expansion do not depend  on temperature.  For moderate temperatures,
            this  is  a  reasonable  approximation.  This  conclusion  follows  from  Fig. 7.6  in
            which experimental results  of Sukhanov et al. (1990) (shown with  solid lines) are
            compared with Eqs. (7.20), where AT  = T - 20°C (broken lines) for carbon-poxy
            angle-ply laminates. However, for relatively high temperatures, some deviation from
            the  linear  behavior  can  be  seen.  In  this  case,  Eqs. (7.13) and  (7.20)  for  thermal
            strains can be generalized as


               cT  = 1a(T)dT .

                    77,
            Temperature action can result also in the change of material mechanical properties.
            As follows from Fig. 7.7 in which circles correspond to experimental data of Ha and
            Springer (1 987), elevated temperature causes higher or lower reduction of material
            strength  and  stiffness  characteristics  depending  on  whether  the  corresponding
            material characteristic is controlled mainly by the fibers or by the matrix. The curves
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