In mathematics, given a metric tensor , a covariant derivative is said to be compatible with the metric if the following condition is satisfied:
Although other covariant derivatives may be supported within the metric, usually one only ever considers the metric-compatible one. This is because given two covariant derivatives, and , there exists a tensor for transforming from one to the other:
If the space is also torsion-free, then the tensor is symmetric in its first two indices.