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Hot-Rolled Strip Laminar Cooling Process with Distributed Predictive Control  241


                         7.5 m                  62.41m            7.5 m
                                  5.2 m
                                       Water cooling section
                   X-ray
                                                                             Pinch roll



                     Pyrometer
               Finishing mill                                                  Coiler
                                       Main cooling section   Fine cooling section

                              Figure 11.1  Hot-rolled strip laminar cooling process


             section. In this HSLC, the number of cooling water header groups and the water flux of each
             header group are taken as control variables to adjust the temperature distribution of the strip.



             11.2.2  Thermodynamic Model

             Consider the whole HSLC process from the point of view of geometrically distributed setting
             system (the limits of which are represented by the geometrical locations of FT and CT, as
             well as the strip top and bottom sides), a two-dimensional mathematical model for Carte-
             sian coordinates is developed combining academic and industrial research findings [126].
             The model assumes that there is no direction dependency for the heat conductivity   . There
             is no heat transfer in traverse and rolling direction. The latent heat is considered by using
             temperature-dependent thermal property developed in [127] and the model is expressed as

                                                  2
                                              −      x    x
                                           ̇ x =     − l ̇                        (11.1)
                                                c   z 2    l
                                                p
             with the boundary conditions on its top and bottom surfaces
                                               x
                                          ±     = h(x − x )                       (11.2)
                                                       ∞
                                               z
             where the right-hand side of (11.2) is h times (x − x ) and
                                                      ∞
                                                        4
                                            x − x w    x − x 4 ∞
                                      h = h       +                               (11.3)
                                           w         0
                                            x − x       x − x
                                                ∞           ∞
             and
             x(z, l, t) strip temperature at position (z, l),
             l,z length coordinate and thickness coordinate, respectively,
                density of strip steel,
             c specific heat capacity;
              p
                heat conductivity,
                                                       4
                                                    2
                Stefan–Boltzmann constant (5.67 × 10 −8  W/m K ),
              0
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