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Modeling and optimal control of cancer-immune system  97


                          yðtÞ¼ ψðtÞ,t 0  τ max   t < t 0 , and yðt 0 Þ¼ y 0 :  (A.2)
              It should be noted that ψ(t 0  ) need not be the same as y 0 . This immediately
              introduces the possibility of a discontinuity in the state, y(t).
                 We mention here that there are many problems in biosciences (such as
              epidemics, harvesting, chemostats, treatment of diseases, physiological con-
              trol, vaccination) that can be addressed within an optimal control framework
              for systems of DDEs (Banks, 1975; Kolmanovskii and Shaikhet, 1996;
              Smith, 2005). However, the amount of real experience that exists with
              OCPs is still small. The DDE (A.1) can be converted into an OCP by adding
              an m-dimensional control term u(t)
                        0
                       y ðtÞ¼ fðyðtÞ,yðt τ 1 Þ,yðt τ 2 Þ,…,yðt τ d Þ,uðtÞ,tÞ  (A.3)
              and a suitable objective functional (measure): J 0 (u)

                                 t f
                               Z
               Minimize J 0 ðuÞ¼  LðyðtÞ,yðt τ 1 Þ,yðt τ 2 Þ,…,yðt τ d Þ,uðtÞ,tÞdt,
                                0
                                                                          (A.4)
              and subject to control constraint a   u(t)   b, and state constant y(t)   c,
              where a and b are the lower and upper bounds. The integrand, Lð:Þ is called
              the Lagrangian of objective functional, which is continuous in [0, t f ]. Addi-
              tional equality or inequality constraint(s) can be imposed in terms of J i (u).
                 Pontryagin’s maximum principle (Pontryagin et al., 1962)gives
              necessary conditions that the control and the state need to satisfy, and
              introduces an adjoint function to affix to the differential equation to the
              objective functional. The necessary conditions needed to solve the
              OCP are derived from the so-called “Hamiltonian” H,which is given
              by the equation

                                                 T
                                    HðtÞ¼Lð:Þ + λ ðtÞfð:Þ                 (A.5)
                    T
              Here, λ (t) is a vector of costate variables of the state variables y(t), which is
              the solution of the equation

                         ∂H                ∂H
                 0           ðtÞ χ
                λ ðtÞ¼                          ðt+ τÞðAdjoint equationÞ  (A.6)
                                   ½0, t f  τŠ
                        ∂yðtÞ           ∂yðt τÞ
              where

                                           1   if t   ½0, t f  τŠ
                                χ      ¼
                                 ½0, t f  τŠ
                                           0   otherwise
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