An affine parameter on a geodesic is one for which the coordinate equation has the form x¨k+Γijkx˙ix˙j=0. Its affine changes λ↦Aλ+B, with A=0, preserve this form.
An affine parameter on a timelike geodesic can be scaled to proper time. With metric signature (+−−−) this fixes the tangent-vector norm to c2. A further constant rescaling preserves the affine geodesic equation but changes that norm; conserved energy and angular-momentum constants must be rescaled consistently. The unit term in a proper-time-normalized radial energy equation is consequently a normalization choice, not a property of every affine parameter.
A change λ↦Aλ+B rescales a geodesic tangent and all its linear Killing constants by 1/A. A null norm remains zero and cannot fix A, unlike proper-time normalization of a material particle. Ratios of the constants, such as the photon impact parameter b=∣h∣/(ck) in Schwarzschild spacetime, are independent of the affine scale. A physically normalized four-momentum fixes the photon energy and hence selects a tangent scale.
For physical four-momentum Pμ=mdxμ/dτ, the covariant-component equation is dPμ/dτ=(∂μgνσ)PνPσ/(2m). The equation without 1/m instead uses a tangent parametrization, or the affine parameter λ=τ/m when the tangent is the physical momentum.
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- Affine connection for a velocity-linear force
- Affine focusing model for the Penrose theorem
- Affine momentum normalization of a geodesic
- Affine normalization in a Kaluza-Klein geodesic reduction
- Affine parameter change under conformal rescaling
- Affine-time scaling of a nonradial Schwarzschild photon plunge
- Conformal Killing geodesic identity
- Conformal preservation of null geodesic paths
- Energy-normalized angular momentum for a Schwarzschild geodesic
- Equatorial Kerr null geodesic radial equation
- Extendible geodesic
- Geodesic
- Geodesic conserved quantity from a Killing vector
- Geodesic endpoints in Minkowski conformal compactification
- Geodesic reparametrization under projective equivalence
- Geometrization of the Lorentz force by an affine connection
- Newtonian connection from an exponential lapse
- Null effective potential in Schwarzschild spacetime
- Null geodesic incompleteness
- Null infinity
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- Penrose singularity theorem
- Penrose theorem at a Cauchy horizon
- Pregeodesic
- Projective equivalence of affine connections
- Proper-time normalization of an affine parameter
- Radial null geodesics of the Vaidya metric
- Rindler null geodesics
- Spacelike geodesic
- Timelike geodesic
- Timelike length and energy have the same geodesic images
- Trapped surface
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