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  1. #1
    Raider of the lost time
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    secret of centripetal force

    For all uniform circular motion, the magnitude of the velocity vector is a constant even though its direction is changing continuously. When this direction points along the same orientation again it can only indicate a complete cycle. However, for the centripetal force to be exactly radial, the instantaneous change in time must be taken to the limit using the formalism of differential calculus such that ∆t ® 0, implying its time independence. In addition to being mass independence the scalar product of centripetal acceleration and radius vector is a constant square of light speed.
    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: secret of centripetal force

    Antonio,great thread starter,seems to have been overlooked though,We shall changs that right now,what do you saqy to that suggestion my friend?

    The secret maybe that one and the other are the two primary forces of universal
    matter substantiation,Ying and Yang,the two primal spinners of form?

    Just an idea Antonio,can it be developed??

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

  3. #3
    The Thinker
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    Re: secret of centripetal force

    Quote Originally Posted by AntonioLao View Post
    However, for the centripetal force to be exactly radial, the instantaneous change in time must be taken to the limit using the formalism of differential calculus such that ∆t ® 0, implying its time independence.
    In my thought, if something exists in time it must exist in space, and vice versa. So if something is time independent then it must necessarily be space independent too. Something which is both time and space independent doesn't exist, I think youa gree on this. But in your theory something can be time independent and not be space independent and vice versa, how is that? I mean, how can something exist in time and not in space, or exist in space and not in time?

  4. #4
    Raider of the lost time
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    Re: secret of centripetal force

    Just got the chance to reply to these posts.
    Quote Originally Posted by Guille
    how can something exist in time and not in space, or exist in space and not in time?
    If we plot space and time against each other as rational functions then s=t/1+t or t=s/1-s, there are three possible solutions sets (s,t) ----> (0,0), (1, infinity), (infinity, 1).
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  5. #5
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    Re: secret of centripetal force

    At the same time,how can time and space exist without any thing. Anything to exist needs space and time. To put it other way, talking time and space without anything i.e. mass /energy is nothing but goobledegook.

  6. #6
    Raider of the lost time
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    Re: secret of centripetal force

    Quote Originally Posted by gautam
    how can time and space exist without any thing.
    In quantum field theories, space and time are the fundamentals ingredients for anything else to exist. I am searching for a formulation that would possibly quantized space and time and consequently it could explain how matter and energy are derived from space and time.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  7. #7
    The Observer
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    Re: secret of centripetal force

    In order to accomplish such a mathematical feat Antonio, I believe you would need to give time and space physical attributes. Einstein did it and called it General Relativity.
    David

  8. #8
    Raider of the lost time
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    Re: secret of centripetal force

    Quote Originally Posted by dleviwing
    Einstein did it and called it General Relativity.
    If Einstein is here with us today, a second guess is he would call his theory general gravity or maybe universal gravity. Still in the quantum field region, there is no gravity since this infinitesimal region is dominated by the strong nuclear force of gluons.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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