Page 102 - Handbook of Materials Failure Analysis
P. 102

2 Physical Nonlinearity of Materials   97




                     The state of elongation at a given point is represented by the equivalent strain, as
                  follows:
                                            q ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
                                                 2    2     2
                                         ε ¼  ðÞ + ε 2 +  ðÞ                     (5.1)
                                                    ðÞ + ε 3 +
                                              ε 1 +
                          ðÞ
                  in which ε i +  corresponds to the positive components of the main strain tensor.
                  These components are defined by: ε i +  ½        ðÞ ¼ ε i if ε i > 0or
                                               ðÞ ¼ ε i + ε i jjŠ=2 with ε i +
                  ðÞ ¼ 0if ε i   0.
                   ε i +
                     The criterion used to verify the material mechanical integrity is defined by:


                                             f ¼ ε  S DðÞ < 0                    (5.2)

                  The variable S DðÞ represents the limit strain value as a function of the damage state.

                  At the beginning of the incremental-iterative process, S DðÞ corresponds to the

                  normal strain value of concrete tensile strength, ε d0 . For the following steps, S DðÞ

                  is updated considering the value of ε determined on the last converged load step, which
                  accounts for the updated damage state. Due to the nonsymmetric mechanical beha-
                  vior of concrete when subjected to tensile and compressive stresses, the damage
                  variable is composed by the sum of two independent parts: tensile portion, D T ,
                  and compressive portion, D C . Each of these portions indicates tensile and compres-
                  sive contributions to the local strain state. These portions are obtained as a function
                  of the equivalent strain and the internal parameters of the damage model, which are
                  defined by:
                                                ð
                                              ε d0 1 A T Þ  A T
                                       D T ¼ 1

                                                 ε      e ½ B T ε ε d0ފ
                                                           ð
                                                ð
                                              ε d0 1 A C Þ  A C
                                       D C ¼ 1                                   (5.3)
                                                 ε      e ½  B C ε ε d0ފ

                                                           ð
                  in which ε d0 ,A T ,B T ,A C ,B C are the internal parameters of Mazars’ damage criterion.
                  The subscripts T and C indicate tensile and compressive parts, respectively.
                     After the determination of each portion of damage, the final value of the damage
                  variable is composed as follows:
                                             D ¼ α T D T + α C D C               (5.4)
                  The coefficients α T and α C are calculated using the following expressions:
                                           X            X
                                              ð ε T i +    ð ε C i +
                                                Þ
                                                             Þ
                                            i            i
                                       α T ¼      , α C ¼                        (5.5)
                                              ε V +        ε V +
                                  are determined from the main stresses considering elastic mate-
                  in which ε T i  and ε C i
                          +
                  rial and ε represents the total state of elongation, which is equal to:
                         V
                                             X        X
                                          +
                                                  Þ +
                                                           Þ
                                         ε ¼    ð ε T i +  ð ε C i +             (5.6)
                                          V
                                              i        i
                  After the damage variable determination, the stress state for the structure (solid) is
                  calculated as follows:
                                              σ ¼ 1 DÞEε
                                                 ð
                                              τ ¼ 1 DÞGγ                         (5.7)
                                                 ð
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