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AntonioLao
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11-05-2005, 06:29 PM
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The Riemann tensor of general relativity is that of differential geometry. The other Riemanns are from number theory.
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Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²
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