Page 329 - The Final Appeal to Mankind

«The Final Appeal to Mankind» by Nicolai Levashov

Given extensive breeding, equation (3) is less than one (1).

Extensive breeding occurs when the vegetative biomass produced by photosynthesis
has not been completely consumed by the herbivorous animals.

Equation (3) represents the system in balance. Fluctuations in the population density
can be represented in the following form:

(-)
(+)
m(t) / N m(n) < 1 < m(t) / N m(n) (4)
What, then, happens within the population that brings equation (4) to (the status of)
equations (5) and (6)?

(+)
m(t) / [N – (β ± Δn)] m(n) → 1 (5)
(-)
m(t) / [N – (p ± Δn)] m(n) → 1 (6)
Let us now try to provide a logical explanation for this phenomenon.

Each individual in the species generates a psi-field; the psi-field generated by one
individual is ω. Psi-fields generated by individuals in the population interact with one
another and affect the processes occurring in their organisms. Let us assume that there
is a certain optimum density of the aggregate psi-field of the population which ensures
optimum conditions of existence for each individual.

W = ∫ ∫k(N;s)ωdsdN (7)
n s

where:

W — is the aggregate psi-field of the population .

S — is the area of the population's habitat.

ω — is the psi-field generated by one individual of the species.

k(N, S) — is the factor representing the mutual effect of the influence of psi–fields
within a population.

Let us introduce a new parameter:

Pw = [ ∫ ∫k(N;s)ωdsdN] / ∫ds = W/S (8)
n s s

where:

Pw — is the optimum density of the aggregate psi–field per unit of surface area given
an optimum population.

In the same way that we obtained equation (4) we can arrive at the following equations:

[ ∫ ∫k(N;s)ωdsdN] / ∫ds < W/S (9)
(-)
N s s

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