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Examples
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There has been a resurgence of interest in Lorentzian relativity.
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There has been a resurgence of interest in Lorentzian relativity.
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One of the underlying assumptions of general relativity is that spacetime can be represented by a Lorentzian manifold with signature (+, -, -, -) or (-, +, +, +) – where the signature of a metric tensor is just the number of positive and negative eigenvalues of the corresponding real symmetric matrix once it is diagonalised.
Bad Language: Metric vs Metric Tensor vs Matrix Form vs Line Element 2009
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A very important thing to remember: The dark star calculations are done for a three-dimensional Euclidean space, while the black hole calculations are done for a four-dimensional Lorentzian spacetime (there is a big difference between the two).
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The Lorentzian manifold is a pseudo-Riemannian manifold, the generalization of the Riemannian manifold, such that the metric tensor need not be positive-definite.
Bad Language: Metric vs Metric Tensor vs Matrix Form vs Line Element 2009
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What is NOT a Riemannian manifold is the familiar Lorentzian manifold of general relativity (of which the Minkowskian manifold of special relativity is a special case).
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The Lorentzian manifold is a pseudo-Riemannian manifold, the generalization of the Riemannian manifold, such that the metric tensor need not be positive-definite.
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General Relativity applies on Lorentzian manifolds, of dimension greater than two.
“On the Origin of Gravity and the Laws of Newton” by Erik Verlinde 2010
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General Relativity applies on Lorentzian manifolds, of dimension greater than two.
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One of the underlying assumptions of general relativity is that spacetime can be represented by a Lorentzian manifold with signature (+, -, -, -) or (-, +, +, +) – where the signature of a metric tensor is just the number of positive and negative eigenvalues of the corresponding real symmetric matrix once it is diagonalised.
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