Calculations on non-classical systems of the type mentioned in the title have been carried out using the treatment described in Part I. As before chain transfer has been neglected. It is shown that the properties of the total pre-effect DELTAM(pre) are analogous to those previously deduced for the after-effect. Thus, for given rates of chain-starting in the initial and final stationary states, the following proportionalities are found: DELTAM(pre) proportional-to (k(p)M)(1+beta)/(1-beta)/k(to)1(1-beta), DELTAM(pre) proportional-to k(p)MR1p2. and DELTAM(pre) proportional-to k(p)MR2p2.. R1. and R2. are the initial and final radical concentrations, beta is the geometric mean exponent in the relation between termination coefficient and radical size and other symbols have their conventional meanings. Non-classical polymerizations with intermittent initiation of the ''rotating sector'' type (light and dark rates of initiation l2p, l2a, respectively) have been treated by the same procedure. Plots of the ratio omegaBAR/omega(s)(omegaBAR = mean rate of polymerization and omega(s) = rate with continuous full rate of initiation) against t(l)/tau have been constructed (t(l) = duration of ''light'' period, tau = mean life-time of chains) for beta = 0.1, beta = 0.139 and beta = 0.2. It is shown that, for given beta and with l2a = 0, omegaBAR/omega(s) is a single-valued function of t(l)/tau. The resulting curves, although resembling those for classical systems, are displaced from the latter; moreover, members of different families (different beta) are not superposable. Systems with intermittent initiation together with a constant background (thermal) initiation and beta = 0.1 and beta = 0.2 have been investigated similarly. Applications to the evaluation of absolute rate coefficients are discussed.