A null curve has tangent satisfying . It represents the possible spacetime path of a light signal.
Its nonzero tangent is a null vector at every regular point; this distinguishes the curve from a single null direction.
A null geodesic is both a null curve and a geodesic. In geometric optics, light rays follow null geodesics.
In a flat two-dimensional Penrose diagram, a straight line tangent to a null vector; with radial metric tensor it is or . Such lines represent radial null geodesics after a conformal transformation.
A radial null geodesic in a spherically symmetric spacetime has zero angular momentum and fixed angular coordinates. Its projection is a null curve of the two-dimensional radial Lorentzian metric.

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