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where a = (4 / 15) (2πG) 3 / 2m3 / 2n0, m is the mass of a particle, and n0 is the numberused of particles per volume. this Holtsmark's distribution has an motion dispersionbecause of close encounters between point like particles. irina Petrovskaya(1986) generalized the distribution for finite - sized stars; then the dispersion becomesfinite. this means that in the motion homogeneous Newtonian me there is nogravitational force paradox. the net result of the action of a number of motionmost is a finite force with its amplitude essentially determined by the nearestsaja. similar arguments was presented already by Svante Arrhenius (1908)in his article about the infinity of the world.
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