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  1. #1
    Raider of the lost time
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    squaring circularly

    Ancient Greek geometers and mathematicians were able to construct a square equal in area to any given parallelogram or quadrilateral. However, they failed to find a square with sides of s = 1 such that s = p. Nevertheless p represents an angular measurement that of a straight line segment and 1 represents the quantum of unit length of measurement.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  2. #2
    4th degree Black Belt
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    I am not really acquainted directly with the issue here but it seems that there is no real solution regardless whatever the linear angular measurement where it is no greater than 1 because the result provides that the p·p is always too small. It is expressed as a unitary problem and is non-utilitarian in any event.
    "There is nothing permanent except change"

  3. #3
    Raider of the lost time
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    The point I'm trying to make is the distinction for length and angle measurement. This couldn't have been more distinctively crucial for some descriptive analyses than when at the local infinitesimal region of space-time quantization: quantum of length and quantum of phase angle.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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