Symbol T_ij
j is part of the quantity the equation computes from the expression on the right.
Read this term in its guide →Published equation contexts
Define the network’s curvature-diagnosing observable directly from this result, restoring physical units through the relation between coordinate acceleration and proper time for a static observer, . a symmetric rank-two tensor in the local spatial frame of the static observers, with units of inverse time squared — the Eötvös units already standard in gravity-gradient surveying, where 1\, = 10^{-9}\, . Under a rotation of the local spatial axes it transforms as an ordinary rank-two tensor; under a change of which node is used as the additive reference for it is unchanged, because it depends only on derivatives of , never its value; and up…
j is part of the quantity the equation computes from the expression on the right.
Read this term in its guide →phi_,ij is one of the signed contributions combined to compute the quantity on the left.
Read this term in its guide →phi_,i is one of the signed contributions combined to compute the quantity on the left.
Read this term in its guide →phi_,j is one of the signed contributions combined to compute the quantity on the left.
Read this term in its guide →Read it with the definitions, units, and assumptions supplied by the article.
A symbol can carry a different meaning in another article. Each occurrence keeps its own guide and term definitions.
Equation 100 · Evolutionary Physics
This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.
Define the network’s curvature-diagnosing observable directly from this result, restoring physical units through the relation between coordinate acceleration and proper time for a static observer, . a symmetric rank-two tensor in the local spatial frame of the static observers, with units of inverse time squared — the Eötvös units already standard in gravity-gradient surveying, where 1\, = 10^{-9}\, . Under a rotation of the local spatial axes it transforms as an ordinary rank-two tensor; under a change of which node is used as the additive reference for it is unchanged, because it depends only on derivatives of , never its value; and up…
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