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  "body": "\n## Summary\n\nThe torsion tensor of an [[affine connection|JX65KSVHSJ]] measures how far covariant derivatives are from being symmetric in the two vector fields.\nThe Lie bracket is subtracted to make this a tensor.\nIt is a tensor field of type $(1, 2)$, antisymmetric in its two arguments.\nConnections with zero torsion are called torsion-free or symmetric; the Levi-Civita connection is the unique torsion-free connection compatible with a given Riemannian metric.\nGeometrically, torsion describes how infinitesimal parallelograms built by parallel transport fail to close.\n\n## Explanations\n\n### L1 human\n\nStart at a point, move a little in direction $X$, then a little in direction $Y$, carrying each direction along with the connection.\nDo the same in the other order.\nFor a torsion-free connection the two endpoints agree to second order, so the small parallelogram closes.\nTorsion measures the small gap that remains.\nThe flat connection of the plane has no torsion, while a connection that twists directions as you move, like a screw, can have torsion.\n",
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