Page 114 - 20dynamics of cancer
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THEORY I                                                     99

                                     i
                              e −ut (ut) /i! for i = 0,...,n − 1, with the initial condition that x 0 (0) = 1
                              and x i (0) = 0 for i> 0. Note that the x i (t) follow the Poisson distribu-
                              tion for the probability of observing i events when the expected number
                              of events is ut.
                                In the multistage model above, the derivative of x n (t) is given by
                              ˙ x n (t) = ux n−1 (t).  From the solution for x n−1 (t), we have ˙ x n (t) =
                              ue −ut (ut) n−1 /n − 1!. Age-specific incidence is
                                                                          n−1
                                               ˙ x n (t)   ˙ x n (t)  u(ut)  /n − 1!
                                       I(t) =         =  n−1     =    n−1   i    ,    (6.2)
                                             1 − x n (t)     x i (t)       (ut) /i!
                                                          i=0           i=0
                              and log-log acceleration from Eq. (5.3) is
                                                  dI (t) /I (t)
                                         LLA (t) =          = n − 1 − ut (S n−2 /S n−1 ),  (6.3)
                                                    dt/t
                                         k     i
                              where S k =  i=0 (ut) /i!.
                                The total fraction of the population that has suffered cancer by age
                              t—the cumulative probability—is

                                                    x n (t) = 1 − e −ut S n−1 .         (6.4)
                                This analysis does not explicitly follow causes of mortality other than
                              cancer. Frank (2004a) analyzed the case in which each stage has a con-
                              stant transition rate to the next stage, u, as above, and also a constant
                              mortality rate from other causes, d. With constant mortality, d, the only
                                                                                          i
                              change in the solution arises in the expression x i (t) = e −(u+d)t (ut) /i!
                              for i = 0,...,n − 1, in particular, with extrinsic mortality, we must
                              use e −(u+d)t  in the solution rather than e −ut . Because these exponen-
                              tial terms arise in both the numerator and denominator of the expres-
                              sion for incidence and so cancel out, extrinsic mortality does not affect
                              the incidence and acceleration solutions given here. The classes x i for
                              i = 0,...,n − 1 can be interpreted as those individuals alive and tumor-
                              less at different stages in progression.

                                                       CONCLUSIONS
                                This simple model shows the tendency of incidence to increase with
                              age in an approximately linear way on log-log scales. The increase in
                              incidence with age occurs because individuals progress through multi-
                              ple precancerous stages. Many processes cause departures from log-log
                              linearity. The following sections explore some of the ways in which pro-
                              gression affects the shape of the age-incidence curve.
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