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The thorny way of truth - Free Energy Community

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v^pf-ivH - 18 - - f^rinovphysicalconclusions.All experimentalists who have measured the pushing force acting on a n-form Amperebridge with different character and geometry <strong>of</strong> the sliding contacts (Moyssides andPappas^ K P- Graneau and P. N. Graneaa, Peoglos^ 'y Marinov^ ') have received figures2higher than 0.5 gN/A . <strong>The</strong> most careful experiment, according to me, has been carriedout by Peoglos^ ' and his figure, if extrapolated to a Il-form bridge with very long legs,is ^1^= I ^ 0.05 pN/A^.My experiment was done very'quickly with a primitive technique and its eventual measuringerror was pretty big' ^ ; the figure obtained by me for the pushing force actingon my n-form bridge was f. = 5 i" 2.5 yN/A .With my Rotating Ampere Bridge with Sliding Contacts' * K I measured the pushingforce acting on a n-form Ampere bridge indirectly and the figure obtained was a little2bit less but near to f . = 5 yN/A .Now the following very important question is to be answered: Will the force pushingan Ampere bridge with very long legs depend on the form <strong>of</strong> the bridge?If we would assume that the above calculation <strong>of</strong> the force acting on a U-form Amperebridge corresponds to physical reality, then the answer will be: yes. Indeed, let us makea n-form bridge with length <strong>of</strong> the shoulder, a, connecting it to the two very long legswith two fourth-circular arcs <strong>of</strong> small radii R. <strong>The</strong> pushing force acting on this bridgewill be bigger than the force with which the legs act^the shoulder; the last force, forI=1A, is(«-')(^A'shoulderIt is clear that, at suitably small R, one can make al<strong>way</strong>s= i^^^^m'^^- d^)(fA)n-forn, ^ (^A)shoulder > ^hh-foa.' "' ^"Z*'' "•For example, if P = e' a = 6.7x10" a, what is an easily realisable bridge, saya = 1000 mm, R = 6.7 mm, we shall have(Vshoulder = 2^>'''''"'«') = »""/*'• ('«'Thus, by making a rectangular loop, the one end <strong>of</strong> which has a U-form, we should beable to set this loop in motion by the action <strong>of</strong> its internal forces, as the pushingforces on its n- and U-form extremities will be not equal.

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