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Thread: Q v d

  1. #1
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    Q v d


    Quantum vacuum displacement (QVD) is an extension of Maxwell’s displacement current in the classical spacetime continuum. This displacement is connected to the magnetic vector potential where and when its magnitude is practically zero while its directions approach infinity. Infinity of directions is equivalent to a mechanical system with infinite degrees of freedom. Since the magnitude of each of the infinite null vectors vanishes, these infinite degrees of freedom become localized at the infinitesimal region of the spacetime continuum. Furthermore, as squares of energy they become integrable using a double least action principle of the squares of the local Lagrangian or squares of the local Hamiltonian or the product of the local Lagrangian and the local Hamiltonian. These three integrable options L, H, and LH could help solve the mystery of cold fusion.

    From an engineering perspective the local infinitesimal energy threshold must be comparable to the mass-energy equivalent of six Ws vector gauge bosons which is about 482 GeV. Consequently, the laser trigger’s energy must be more than 482 GeV and this must be delivered into a region of the spacetime continuum of about a few orders of Planck length.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  2. #2
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    Smile Re: Q v d

    Ths answer to cold fusion lies I am sure in the recognision
    and understanding the unification of consciousness as the
    primary and only real "thing" there is! When this understanding is "squared" and etheric laws are understood
    as well as physical laws,then cold fusion and the answer
    to it,"will automatically arise within the focussed intent
    of the individual" such is the law!



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

  3. #3
    Raider of the lost time
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    Re: Q v d

    The square of relative consciousness is the absolute consciousness.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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