The recently formulated metabolic theory of ecology has profound implications for the evolution of life histories. Metabolic rate constrains the scaling of production with body mass, so that larger organisms have lower rates of production on a mass-specific basis than smaller ones. Here, we explore the implications of this constraint for life-history evolution. We show that for a range of very simple life histories, Darwinian fitness is equal to birth rate minus death rate. So, natural selection maximizes birth and production rates and minimizes death rates. This implies that decreased body size will generally be favored because it increases production, so long as mortality is unaffected. Alternatively, increased body size will be favored only if it decreases mortality or enhances reproductive success sufficiently to override the preexisting production constraint. Adaptations that may favor evolution of larger size include niche shifts that decrease mortality by escaping predation or that increase fecundity by exploiting new abundant food sources. These principles can be generalized to better understand the intimate relationship between the genetic currency of evolution and the metabolic currency of ecology.allometry ͉ life-history theory ͉ metabolic ecology T he recently formulated metabolic theory of ecology (1) predicts that many attributes of individuals, populations, communities, and ecosystems should be relatively straightforward consequences of the metabolic processes of the relevant organisms. Specifically, many rate processes should scale with body size and temperature in the same way as mass-specific metabolic rate:where R is the rate of some biological process, R 0 is a normalization constant, the M Ϫ1/4 term gives the power-function dependence on body mass M, and the e ϪE/kT term or Boltzmann factor gives the exponential temperature dependence in terms of an ''activation energy'', E, Boltzmann's constant, k, and temperature, T, in Kelvin. This very general relationship holds both within and between species. It can be applied to the rate of production of biomass per unit mass, which is predicted to scale as M Ϫ1/4 (e.g., refs. 2-4). If we ignore temperature or assume for the moment that it does not vary, the Boltzmann factor is a constant. Then, taking logarithms of Eq. 1 we have log (mass-specific production rate)
log (body mass). [2]This prediction appears to be generally supported, although for some traits, the empirically measured scaling exponents appear to deviate from the predicted Ϫ1͞4, sometimes being closer to Ϫ1͞3 (e.g., ref. 5). For our argument here, however, the exact value of the exponent is not an issue; what is important is that it is negative. The consequence of the negative exponent is that in a log-log plot, mass-specific production rate is a declining straight-line function of body mass, as shown schematically by the solid black line in Fig. 2 A. We take this to be a fundamental causal constraint limiting life-history options as suggested by metabolic theory. The result is that sm...