Einstein’s equations,
, represent ten independent equations. Since there are ten equations
and ten independent components of the 4-metric
, it seems that we have the same number of equations
as unknowns. From the definition of the Einstein tensor (3
), we see that these ten equations are linear in the
second derivatives and quadratic in the first derivatives of the metric. We might expect that these ten
second-order equations represent evolution equations for the ten components of the metric. However, a close
inspection of the equations reveals that only six of the ten involve second time-derivatives of the
metric. The remaining four equations are not evolution equations. Instead, they are constraint
equations. The full system of equations is still well posed, however, because of the Bianchi identities
If we consider Einstein’s equations as a Cauchy
problem1,
we find that the ten equations separate into a set of four constraint or initial-value equations, and six
evolution or dynamical equations. If the four initial-value equations are satisfied on some spacelike
hypersurface, which we can label with
, then the Bianchi identities (4
) guarantee that the evolution
equations preserve the constraints on neighboring spacelike hypersurfaces.
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