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  1. #1
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    weak fusion


    Traditional cold fusion would likely be accomplished by this nuclear reaction: D+D®He+energy without using a process of simultaneous increase in plasma density and pressure based on a theory of pseudorandom collisions. The Ds denote deuterons of hydrogen isotopes called deuterium (nucleus of 1 proton and 1 neutron) which is a key component of heavy water D2O. However, a more direct approach is simple electrolysis of ordinary pure water H2O into isolated hydrogen gas H2 and oxygen gas O2. Furthermore, the H2 can then be ionized into positive ions H+ or protons without those binding electrons. A single proton (according to quantum chromodynamics) is a composite of 2 up quarks and 1 down quark. Moreover, quarks are the only elementary particles that are capable of interacting with all 4 fundamental forces of nature (nuclear strong-weak, electromagnetic and gravity). Nevertheless, it is their proximate affinity with the weak force that could be used to initiate a cold weak fusion by direct irradiation with high power lasers whose output energies must be comparable or exceed the mass-energy equivalence of weak gauge vector bosons: ±W.

    Electroweak theory predicted the mass-energy equivalence of ±W to be ~80 GeV (billion electron volts). A high powered laser with this energy would definitely transform 1 up quark of the proton into a down quark, where and when it absorbed the photon conversion to an artificial W-minus gauge vector boson and the proton becomes a neutron. Subsequently, the newly created neutron binds with a proton to form a deuteron, where and when 2 deuterons fused into an ordinary helium nucleus plus excess energy. Even though the energy output of weak fusion is only 2.45 Mev (million electron volts), a nuclear efficiency of only .003%, the laser power can, in theory, be achieved by sequential steps of frequency doubling, trebling or quadrupling to reach the extreme magnitude of 20 million billion billions cycles per second of time.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

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    Smile Re: weak fusion

    We need strong cold fusion,not weak.




    regards michael.
    Humilty,coupled with boldness,surprises truth to
    reveal herself?

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    Re: weak fusion

    For almost 100 years researchers have tried strong hot fusion but nothing ever works. Weak fusion is really concentrated hot fusion at the subfermi length intervals.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

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    Smile Re: weak fusion

    Quote Originally Posted by AntonioLao View Post
    For almost 100 years researchers have tried strong hot fusion but nothing ever works. Weak fusion is really concentrated hot fusion at the subfermi length intervals.

    No hot fusion is a non-starter,however cold fusion can and will occur.




    regards michael.
    Humilty,coupled with boldness,surprises truth to
    reveal herself?

 

 

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