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  1. #1
    Raider of the lost time
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    seeing and believing

    Within mathematical limit, seeing and believing are respectively equivalent to projective and conformal transformation.

    In projective geometry the invariance are properties of configurations or shapes, for example, a person remains a person at temporal zero and spatial infinity instead of changing into a whale with no arm and no leg but fin and tail. In conformal mapping, angles and directions remain invariant at spatial zero and temporal infinity, for example, a person facing east remains facing east at temporal infinity. Both attributes of projective and conformal are applicable to the structure of space-time as its homogeneity and isotropy.
    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 east iseast and west is west.

    Quote Originally Posted by AntonioLao
    Within mathematical limit, seeing and believing are respectively equivalent to projective and conformal transformation.

    In projective geometry the invariance are properties of configurations or shapes, for example, a person remains a person at temporal zero and spatial infinity instead of changing into a whale with no arm and no leg but fin and tail. In conformal mapping, angles and directions remain invariant at spatial zero and temporal infinity, for example, a person facing east remains facing east at temporal infinity. Both attributes of projective and conformal are applicable to the structure of space-time as its homogeneity and isotropy.
    Do you always believe what you see!Or see what you want to believe?By the way
    Antonio,If you were on say mars,would there still be east and west!

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

  3. #3
    Raider of the lost time
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    Quote Originally Posted by mkirkpatrick
    Do you always believe what you see!Or see what you want to believe?
    Mathematically speaking, seeing and believing based on the abstractions of M. C. Escher's lithographs.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

 

 

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