Page 382 - Mechanics Analysis Composite Materials
P. 382

Chapter 8. Optimal composite structures        361

            with respect to design variables hi, 4; and multipliers A,  i.e.





            Minimization with respect to I gives, obviously, constraints in Eqs. (8.1) and (8.2),
            while the first two of Eqs. (8.4) yield

               of)().xcos24; +  sin’  +i  +A.~? sin 4;cos 4;)= I  ,            (8.5)

               hiby)[(A,.-  sin 24i +   cos 24~= EI  A;[(&? - E,)  sin 24; + y.yy COS 24;1  .
                                                                               (8.6)

            The solution of  Eq. (8.6) is













            where c is a constant. Substituting   Ivy, and   from these equations into Eq. (8.5)
            and taking into account Eq. (8.2) we get




            This equation has two solutions: oy)= fc.
              Consider  the  first  case,  Le.,  cy)= c.  Adding  up  the  first  two  equations  of
            Eqs. (8.1) and taking into account Eq. (8.3) we have
                   I
               h=-(Nx+iyv)  .
                   C
            Obviously, the minimum value of h corresponds to c = 51,  where 81  is the ultimate
            stress. Thus, the total thickness of the optimal plate is





            Taking now o?  = 81in Eqs. (8.1) and eliminating 81with the aid of  Eq. (8.8) we
            arrive at the following two optimality conditions in terms of  design variables and
            acting forces:
   377   378   379   380   381   382   383   384   385   386   387