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The thorny way of truth - Free Energy Community

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184We know that each nucleus consists <strong>of</strong> protons and neutrons; the difference betweentheir masses is extremely small and this allowed us to neglect it in (5). We do notknow, however, something certain about the charge distribution and the size <strong>of</strong> the neuatron. That is why we are tempted to assume that relation (6) gives generally proportionality between the EES <strong>of</strong> the nucleus and the EES <strong>of</strong> the particles it consists <strong>of</strong>.If we should assume that the protons and neutrons <strong>of</strong> the atomic nucleus build specificconglomerations called clusters, and if we should ascribe to any such clusterits EES, denoting it by R » we can write Rj^ ~ kR , where k is a certain coefficient <strong>of</strong>proportionality. We can then writeA„=kA^, (7)and thus the elementary wave <strong>of</strong> de Broglie <strong>of</strong> the nucleus will be proportional to theelementary waves <strong>of</strong> the clusters <strong>of</strong> which it consists.We would like to call attention to the fact, that our concepts are quite near tothe cluster hypothesis developed lately by not a few investigators.Relation (7) points to the seldom noticed connection between the elementary wave <strong>of</strong>de Broglie (its EES) and the same waves <strong>of</strong> the clusters <strong>of</strong> which it consists. <strong>The</strong> proportionalitybetween them allows to consider (7) from another point <strong>of</strong> view: as ananalogue <strong>of</strong> the connection which must exist between the width <strong>of</strong> the infinitely deeppotential hole, L, and the wavelength. A, <strong>of</strong> an elementary particle closed in it. <strong>The</strong>width <strong>of</strong> the potential hole must be proportional to the wavelength2L = nA,so that the particle would not be able to leave the hole.We have reasons to liken the double value <strong>of</strong> the EES to the width <strong>of</strong> an infinitelydeep potential hole, where the particles <strong>of</strong> which the nucleus consists are closed. Itseems that, in order the nucleus to be stable, in the double width <strong>of</strong> the hole theremust be a whole number <strong>of</strong> times <strong>of</strong> elementary waves <strong>of</strong> these particles2^^= nA^ or 2R,^ = nR^. (8)As an attempt to illustrate the above presented approach, we shall first considerTable 1 presenting the EES, defined after formula (3) <strong>of</strong> the most elementary existinnuclei: proton, p, deuteron, d, and triton, t, which are also among the fundamental

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