Monday, October 5, 2009

Article 6

The mineral magnet following the logic developed should be a structure of which the arrangement should form some helicoidal movements then some whirls permanently, what should drive continually the particles of the two first secondary elements and especially the smallest ones (1), with creating like this a force field; there it should be considered especially some whirls because the attraction between some magnets or with some iron is specially strong, what helicoidal connections can particularly justify. The helicoidal movement in magnet should come from the flow of the particles going out of the atoms constituting it, this flow should have as a cause the decomposition in some straight lines of the cyclic movements present in the atom, decomposition which should provoke the ephemeral feature (relatively to an absolute consideration) of their cycle of existence ( see article 3). The orientation of the flow of emission should be done during the formation of the magnet where all the atoms and parts are orientating themselves (one another) as for the formation of the crystalline networks which form the tremies (from the Latin: trimodia, sort of pyramid hollowed out) of sodium chloride. The particles concerned being the ones which are found in light (in probably some different proportions) their quantity of motion is Q = m * c, and the force field that they form contains a kinetic energy E = ½ * m *c² ; where c is the velocity of light, and m corresponds to the quantity of particles displaced in the flow. The quantity of motion should be considerable in a durable manner in an atom without being maintained, because the movement of light is relatively stable, what should be found as well in this case; otherwise in the majority of cases there is in a non-negligible manner some transmissions of some particles and of their movement to which the kinetic energy gives utterance, besides the atomic energy of fission should come from the rupture of the cycle of a nucleus, which in its energetic liberation should permit among others the production or liberation of some inferior cycles giving the neutron, which could be named intermedion in this system. Also we can notice a particular affinity with iron, and this should be due to the fact that its structure is close to the one of the mineral magnet which is an oxide of iron and its rate of radiation should be as well close to the other one, although it should permit a less dense outflow for each pore and differently arranged in a pore and between the pores, but which is possible to influenced; thus should be produced an attraction by the propagation of the movement in cyclone, acting as a screw, phenomenon which seems as well to be produced with nickel and cobalt, of which the atomic weight are close to the one of iron; generally for the other materials the strength of the flows and the width of the pores should permit to the contact to be done without any particular resistance (2). Besides with some iron it is possible to make an electromagnet out of rolling up a wire of iron around a core of iron by a helicoidal manner (which may not be by chance) and well tight, and out of making pass a flow of some electric particles through it, then of the ones which pass generally in a magnet, with a possible variation in the proportion between the concentrations of the particles of the first and second secondary element (1) according to the type of magnet (electro or mineral). On the top of that we can remark that when the current increases in the electromagnet, some warmth is produced, what confirms the importance of the concentration of the particles of the two first secondary elements for its production; also out of increasing more we can obtain some light which depends especially on the concentration of energy in the form of some malleable particles, then on the type of these particles according to the fractality (see article 2).

(1) : See :
(2): We can all the same note diamagnetism, which generally has a weak effect.

Update 05/04/2011: In order to be sure of the resistance of some helicoidal movements of some particles of the same type as the particles considered for the magnet, which allows here the consideration of a force field, it is possible to read (optical tweezers are interesting here):