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Stresses and strains  17


              1.4.4 Plane stress and plane strain in isotropic thermal
                    rocks
              1.4.4.1 Plane stress state
              Plane stress and plane strain states can simplify 3-D stressestrain relations into
              the corresponding 2-D forms. For a plane stress (biaxial stress) deformation
              state, it has s z ¼ s yz ¼ s zx ¼ 0; therefore, substituting this condition into
              Eq. (1.23) the strainestress relations have the following forms:
                                      1
                                 ε x ¼  ðs x   ns y Þ  a T DT
                                      E
                                      1
                                 ε y ¼  ðs y   ns x Þ  a T DT
                                      E                                  (1.29)
                                        n
                                 ε z ¼  ðs x þ s y Þ  a T DT
                                        E
                                        1
                                 ε xy ¼   s xy
                                       2G
              and from Eq. (1.24) stressestrain relations can be expressed as follows:
                                      E              Ea T DT
                               s x ¼      ðε x þ nε y Þ þ
                                    1   n 2            1   n
                                      E              Ea T DT             (1.30)
                               s y ¼     2  ðε y þ nε x Þþ
                                    1   n             1   n
                               s xy ¼ 2Gε xy
                 This case occurs when a thin plate is stressed in its own plane. It also
              occurs in the analysis at any free surface, if the x- and y-axes are taken in the
              surface ( Jeager and Cook, 1979).

              1.4.4.2 Plane strain state
              For a plane strain (biaxial strain) deformation state, ε z ¼ ε yz ¼ ε zx ¼ 0;
              substituting this relation into Eq. (1.23) the strainestress relations can be
              expressed as follows:
                               1 þ n
                          ε x ¼     ½ð1   nÞs x   ns y Š   ð1 þ nÞa T DT
                                E
                               1 þ n
                          ε y ¼     ½ð1   nÞs y   ns x Š   ð1 þ nÞa T DT  (1.31)
                                E
                                1
                          ε xy ¼  s xy
                               2G
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