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118                              Entropy Analysis in Thermal Engineering Systems


          Table 8.2 The effect of heat exchanger effectiveness on the maximum thermal
          efficiency and minimum specific entropy generation of the regenerative gas
          turbine cycle.
                          Simple cycle e50.55 e50.65 e50.75 e50.85 e50.95
                          0.370      0.380   0.394   0.415   0.448   0.512
          η max
          SEG min (J/molK) 1771      1741    1705    1652    1567    1403


          TIT¼1273K, η c ¼0.85, and η t ¼0.90. So, the efficiency limit would
          change with a change in TIT, η c ,or η t .
             Fig. 8.6 depicts the distribution of SEG throughout the cycle at the con-
          dition of minimum SEG for three different values of E. Like in the simple gas
          turbine cycle, the combustion process and flue gases cooling are the two
          major SEG contributors. Evident from Fig. 8.6 is that an improvement in
          the effectiveness leads to a reduction in the SEG share of both combustion
          and cooling processes indicating that the thermal energy is utilized more effi-
          ciently. On the other hand, the heat exchanger contribution to SEG
          increases with an increase in the effectiveness, which is due to an increased
          heat transfer within the recuperator. The combined SEG share of the com-
          pressor and turbine remains relatively unaltered. The net reduction in the
          combined SEG share of the combustion and cooling processes exceeds




























          Fig. 8.6 Distribution of the specific entropy generation throughout the regenerative
          gas turbine cycle at minimum SEG for three values of E (TIT¼1273 K, η c ¼0.85, η t ¼0.90).
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