Page 128 - 20dynamics of cancer
P. 128

THEORY I                                                    113

                              multiplied by the clone size, y, so the outflux of that cell lineage from
                              time s to time t is
                                                    t              K i     v i K i /r i
                                        D i (t, s) = e −  s  v i y i (α)dα  =     .
                                                               K i + e i (t−s)  − 1
                                                                    r
                              The total rate of outflux from stage i to stage i + 1 at time t is

                                                       t
                                     u i (t) = v i y (t) = v i  u i−1 (s) D i (t, s) y i (t − s) ds/x i (t) .
                                              i
                                                       0
                              This model is general enough to fit many different shapes of acceleration
                              curves. However, the goal here is not to fit but to emphasize that a few
                              general processes can explain the differences between tissues in their
                              acceleration patterns.
                                Figure 6.9a illustrates the effect of changing the rate of clonal expan-
                              sion, r, in a single round of clonal expansion in stage n − 1, similar
                              to the model of Luebeck and Moolgavkar (2002). Slower clonal expan-
                              sion causes the acceleration in cancer to happen more slowly and to be
                              spread over more years, because slow clonal expansion causes a slow
                              increase in the rate at which a lineage acquires the final transition that
                              leads to cancer. A rapid round of clonal expansion effectively reduces
                              by one the number of steps, n, so that for n = 4, one round of rapid
                              clonal expansion yields a nearly constant acceleration of n − 2 = 2 over
                              all ages (not shown). By contrast, slow clonal expansion often causes a
                              midlife peak in acceleration, as illustrated in the figure.
                                Figure 6.9b shows that an increase in maximum clone size raises the
                              peak level of acceleration until the clone becomes large enough that a
                              transition almost certainly occurs in a short time interval, after which
                              further clonal expansion does not increase the rate of progression.
                                Figure 6.9c shows that multiple rounds of clonal expansion can great-
                              ly increase the peak acceleration of cancer. The curves from bottom to
                              top have one, two, or three rounds of clonal expansion.


                                                       CONCLUSIONS
                                Transition rates that increase slowly over time cause acceleration to
                              rise to a midlife peak and then decline late in life. Clonal expansion may
                              be one way in which transition rates rise slowly over time. Alternatively,
                              somatic mutation rates may increase as various checks on the cell cycle
                              and DNA integrity decay with age.
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