Einstein–Infeld–Hoffmann equations
E811620
approximation scheme in gravitational theory
equations of motion in general relativity
post-Newtonian equations of motion
The Einstein–Infeld–Hoffmann equations are post-Newtonian equations of motion in general relativity that describe the dynamics of gravitating bodies with relativistic corrections beyond Newtonian gravity.
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
approximation scheme in gravitational theory
ⓘ
equations of motion in general relativity ⓘ post-Newtonian equations of motion ⓘ |
| appliesTo |
slowly moving bodies compared to speed of light
ⓘ
weak gravitational fields ⓘ |
| approximates | geodesic motion in curved spacetime ⓘ |
| assumes |
point-mass approximation for bodies
ⓘ
slow-motion approximation v much less than c ⓘ |
| basedOn | Einstein field equations NERFINISHED ⓘ |
| describes |
dynamics of gravitating bodies with relativistic corrections
ⓘ
motion of point-like masses in general relativity ⓘ post-Newtonian corrections to Newtonian gravity ⓘ |
| developedBy |
Albert Einstein
NERFINISHED
ⓘ
Banesh Hoffmann NERFINISHED ⓘ Leopold Infeld NERFINISHED ⓘ |
| excludesEffect | gravitational radiation reaction at leading order ⓘ |
| field |
celestial mechanics
ⓘ
general relativity ⓘ gravitational physics ⓘ |
| generalizationOf | Newtonian N-body equations of motion ⓘ |
| improvesUpon | Newtonian equations of motion ⓘ |
| includesEffect |
finite propagation speed of gravity
ⓘ
gravitational time dilation effects in motion ⓘ periastron precession ⓘ relativistic corrections to orbital motion ⓘ velocity-dependent gravitational interactions ⓘ |
| involves |
expansion in powers of v over c
ⓘ
mass monopole contributions of bodies ⓘ |
| mathematicalForm | coupled ordinary differential equations for particle trajectories ⓘ |
| namedAfter |
Albert Einstein
NERFINISHED
ⓘ
Banesh Hoffmann NERFINISHED ⓘ Leopold Infeld NERFINISHED ⓘ |
| order | first post-Newtonian order ⓘ |
| publicationYear | 1938 ⓘ |
| publishedIn | Annals of Mathematics NERFINISHED ⓘ |
| relatedConcept |
Einstein field equations in weak-field limit
NERFINISHED
ⓘ
parameterized post-Newtonian formalism ⓘ post-Newtonian formalism ⓘ two-body problem in general relativity ⓘ |
| usedFor |
high-precision ephemerides of planets
ⓘ
spacecraft navigation in relativistic models ⓘ |
| usedIn |
binary star orbital calculations
ⓘ
solar system dynamics modeling ⓘ tests of general relativity in weak-field regime ⓘ |
| usesApproximation | post-Newtonian expansion ⓘ |
| validWhen |
gravitational potentials are small compared to c squared
ⓘ
orbital velocities are small compared to speed of light ⓘ |
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.
subject surface form:
Leopold Infeld