Page 93 - The Final Appeal to Mankind
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«The Final Appeal to Mankind» by Nicolai Levashov

            k(N;S)  is  the  coefficient  of  interaction  between  individual  psi-fields  within  the
            population.

            The colony with a higher than optimum population generates a shared psi-field that is

            excessively dense while the colony with a lower than optimum population generates a
            lower-density shared psi-field.

                      (+)
                  ΔW  = ∫∫k(N;S)ωdsdN - ∫∫k(N;S)ωdsdN          (2)  — (greater than optimum density).
                              N+ S           N S
                      (-)
                  ΔW  = ∫∫k(N;S)ωdsdN - ∫∫k(N;S)ωdsdN          (3) — (less than optimum density).
                              N S            N- S
                                                     (+)
            An excessively dense psi-field, ∆W , depresses the physiological processes of each
            individual organism.

            Hormonal  disorders  increase  and  pituitary  and  thymus  activity  become  blocked,
            leading to a decrease in the birth rate and a reduction in life span. A psi-field density
            ∆W , that is too low, stimulates the same processes resulting in an increase in the birth
                 (–)
            rate, etc.

            It is precisely the shared psi-field of the population W, generated by all individual

            species of the population, that is the monitoring mechanism regulating the balance
            between the population of the species and the ecological system.

            The coefficient of interaction, k(N;S), denoting the extent of interaction between the
            psi-fields  within  the  population  is  very  important.  The  coefficient  of  interaction
            depends upon the number of individuals comprising a population and the size of
            the natural habitat occupied by the population. For most species the important range

            is:

            0 < k(N;S) < 1
            There are, however, situations where this parameter can have a negative value or where

            it can be larger than 1 (one). Let us consider the natural phenomena that affect k(N;S)
            causing the values of this parameter to change.

            In  times  of  severe  drought,  when  members  of  different  species  are  in  danger  of
            extinction, an interesting phenomenon takes place. All the individuals of the species
            crowd together, numbering millions, and sometimes billions of individuals (locusts,

            termites, etc.). These population masses, “superorganisms,” with a k(N;S) = 1 manifest
            very  interesting  behaviors.  In  this  situation  the  individual  psi-field  completely
            disappears and is replaced by the shared psi-field of the entire colony. In the case of
            rats and mice, they move in a huge mass, overcoming all obstacles to reach a place
            where there is no drought and where the population can survive. The interesting aspect
            of this phenomenon is as follows:


            a) When the migrating species meets an obstacle like a brook, river, or gully, etc.,
            thousands, and at times, hundreds of thousands fill the obstacles with their bodies and



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