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  1. #1
    Raider of the lost time
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    where when minus one?

    Starting from a single imaginary unit, i, square it, the answer is -1. Taking the slopes of two perpendicular lines, multiply them, the result is also negative unity. These slopes exist only by a prioritized coordinate system. Insert pinto Euler’s equation the imaginary power of the base of natural logarithm becomes negative unity. The square of the product of Pauli’s second spin matrix, s-2 and the imaginary unit also gives the matrix of negative unity. In the theory of infinite series, the negative sum of the infinite sequence ½, ¼, 1/8, 1/16, 1/32, 1/64, etc. is also negative unity. Although the whole number zero separates the real numbers into pluses and minuses it is when minus unity is added to plus unity that proves zero exists (-1+1=0).
    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: where when minus one?

    If you really minused one,you would be left with less than nothing?



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

  3. #3
    Raider of the lost time
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    Re: where when minus one?

    [QUOTE=mkirkpatrick]would be left with less than nothing[/QUOTE]
    Actually a single point has dimension of -1.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  4. #4
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    Smile Re: where when minus one?

    Quote Originally Posted by AntonioLao View Post
    [QUOTE=mkirkpatrick]would be left with less than nothing
    Actually a single point has dimension of -1.[/quote]

    That might be the case,but what would that purchase in the real world?



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

  5. #5
    Raider of the lost time
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    Re: where when minus one?

    Quote Originally Posted by mkirkpatrick
    but what would that purchase in the real world?
    This is the same as purchasing using credit cards on someone else money at borrowing interest.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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