Page 189 - 20dynamics of cancer
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174                                                 CHAPTER 9

                              does of course increase the accumulation of mutations, but does so dif-
                              ferently from the mechanisms by which classical mutagens act. For ex-
                              ample, the potentially mutagenic chemicals in cigarette smoke diffuse
                              widely throughout the body, yet the carcinogenic effects concentrate
                              disproportionately in the lungs. To explain this discrepancy in smok-
                              ers between the distribution of chemical mutagens and the distribution
                              of tumors, Cairns argued that the carcinogenic effects of smoke arise
                              mostly from the irritation to the lung epithelia and the associated in-
                              crease in cell division.
                                If carcinogens sometimes act primarily by increasing cell division,
                              then we would need to know how mitogenic effects rise with dose. For
                              example, doubling the number of cigarettes smoked might not double
                              the rate at which epithelial stem cells divide to repair tissue damage. I
                              do not know of data that measure the actual relation between mitoge-
                              nesis and dose, but, plausibly, mitogenesis might rise with something
                              like the square root of dose instead of increasing linearly with dose.
                                A diminishing increase in transition rates with dose would explain the
                              observation that the exponent on dose is usually less than the exponent
                              on duration. That observation is often expressed with the Druckrey
                              equation that fits data from many studies of chemical carcinogenesis
                              (Figures 2.11, 9.2). The Druckrey equation can be expressed as k =
                                  n
                               r
                              d m , where k is a constant, d is the dose level, and m is the median
                              duration of carcinogen exposure to onset of a particular type of tumor.
                              Usually, r< n, that is, the exponent on dose is less than the exponent
                              on duration. Peto (1977) mentioned that, for carcinomas, r/n is often
                              about 1/2.
                                Now consider a simple multistage model with n stages and equal tran-
                              sition rates, u, between stages. Assume a carcinogen has the same effect
                              on all stages, in which the transition rate is uf(d), where f(d) is a func-
                                                                      n
                                                                    n
                              tion of carcinogen dose, d. Then k = [f(d)] m , because the carcinogen
                              has the same multiplicative effect on all n stages.
                                Suppose that the rise in transition rates diminishes with dose, for
                                              a
                              example, f(d) = d , with a< 1. Then the basic multistage model with
                                                                                 n
                              all n transitions affected by a carcinogen leads to k = d an m .If a = r/n,
                                                                            r
                                                                               n
                              then we have the standard Druckrey relation, k = d m , which closely
                              fits observations from many different experiments with a = r/n ≈ 1/2.
                                Alternatively, we could use the more plausible expression uf(d) =
                                                                                      a n
                                                                                           n
                                      a
                              u(1 + bd ), which leads to the multistage prediction k = (1 + bd ) m .
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