Mass rescaling allometries
The natural selection optimum for density regulation explains the 3/4 and 5/6 exponents of body mass allometries
A large amount of the phenotypic variation across natural species is explained by body mass allometries (Kleiber, 1932; Peters, 1983; Calder, 1984), where traits like mass specific metabolism (β) are given as power functions of mass
β ∝ wb
with the exponent (b) being the slope on double logarithmic scale; ln(β) ∝ b ln(w).
The allometric exponents that describe the mass-rescaling response of the life history to the evolutionary changes in mass are given primarily by the invariant density regulation
fe[εN] ∝ fι[VNH(d-1)/d/fe] ∝ fs[βH1/d/V] ∝ w0
that evolves from the population dynamic feed-back selection on mass.
With foraging speed (V) being proportional with biotic time (T) on the body mass axis (Garland, 1983; Calder, 1984), we may exchange V with T in these functions, and insert power relations wx for the relevant traits in the invariant regulation. Combined with i) the ε=αβ relation between net energy, resource handling and pace, ii) the λ = 1 condition of the population dynamic equilibrium, and iii) the T ∝ 1/β scaling from metabolic trade-off selection, we obtain the following equations for the allometric exponents (see Witting, 1995, 2017 for details):
t + n + (d-1)h/d = 0,
b – t + h/d = 0,
n + e = 0,
t = - b,
e = 1 + b,
a = 1,
p + t + e = 1,
[time periods: T∝wt; abundance: N∝wn; home range: H∝wh; pace and mass specific metabolism: β∝wb; energetic state: ε∝we; resource handling: α∝wa; survival: P∝wp].
When these equations are solved, we obtain the results in Table 1. 1/4 and 3/4 exponents follow from two dimensional interactions (2D; d=2). The corresponding exponents for three dimensional interactions are 1/6 and 5/6, and the exponents are 1/2 for interactions in one dimension.
Evidence
The theoretically predicted exponents for two dimensional interactions are compared with empirical exponents for mammals, reptiles and birds in Table 2.
I have found no convincing 1D cases, but the 2D-3D-transition is supported by taxa from unicells to mammals when grouped according to empirical estimates of exponent for mass specific metabolism (Table 3). Most terrestrial and benthic taxa are classified as 2D, and pelagic taxa and primates as 3D. The 2D-3D transition is also supported by empirical estimates of the exponents for lifespan and population density (Fig. 1 and Table 4).
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References
- Calder, W. A.I. 1984. Size, function, and life history. Harvard University Press, Cambridge.
- Garland, T. 1983. Scaling the ecological cost of transport to body mass in terrestrial mammals. The American Naturalist 121:571--587.
- Kleiber, M. 1932. Body and size and metabolism. Hilgardia 6:315--353.
- Nowak, R.M. 1991. Walker's mammals of the world, volume I--II. 5th ed. The Johns Hopkins University Press, Baltimore.
- Pawar, S., A.I. Dell and V.M. Savage 2012. Dimensionality of consumer search space drives trophic interaction strengths. Nature 486:485--489.
- Peters, R.H. 1983. The ecological implication of body size. Cambridge University Press, Cambridge.
- Witting, L. 1995. The body mass allometries as evolutionarily determined by the foraging of mobile organisms. Journal of Theoretical Biology 177:129--137, https://doi.org/10.1006/jtbi.1995.0231.
- Witting, L. 1997. A general theory of evolution. By means of selection by density dependent competitive interactions. Peregrine Publisher, Århus, 330 pp, URL https://mrLife.org.
- Witting, L. 2017. The natural selection of metabolism and mass selects allometric transitions from prokaryotes to mammals. Theoretical Population Biology 117:23--42, https://dx.doi.org/10.1016/j.tpb.2017.08.005.