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  1. #1
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    permeability

    The general definition of magnetic permeability (m) is the ratio of magnetic flux (lines of force) density (B) in matter to the magnetic field intensity of the surrounding vacuum (H), m= B/H. Since the permeability of the vacuum is a constant number equals p/2500000 henries per meter in SI units this suggests that if the vacuum is considered as a substance analogous to ponderous matter then it does not change the strength of any superset magnetic field of itself.
    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: permeability

    A very interesting idea and thread,however where would magnetism fit into
    a perfect vacuum?In the partial vacuum of our "normal space time"there is an
    interplay of forces within this gulf!But what of the perfect vacuum,"the void"
    would there be any interplay at all here???


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

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    Re: permeability

    I keep thinking that the void is made of equal magnetic helicities. Moreover, these could not be separated into distinct observable helicities like that of positive and negative charged particles.
    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: permeability

    I know what you are saying Antonio,Buthave you ever considered that maybe
    the "void" is absolutely DE_VOID of any interplay or force at all?Now there may well be "potential" but it is absolutely un-realized,and there fore
    undetectable,and unknown!
    I eagerly await your response.


    kindest regards michael.
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    reveal herself?

  5. #5
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    Re: permeability

    Quote Originally Posted by mkirkpatrick
    the "void" is absolutely DE_VOID of any interplay or force at all
    In the void can be found the infinitely powerful orthogonal primary forces of equal absolute magnitudes but opposite in directions. They are not responding to our probings.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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