Einstein–Maxwell equations
E78014
equations of motion
field equations
system of partial differential equations
theory in theoretical physics
The Einstein–Maxwell equations are the coupled set of field equations in general relativity that describe how spacetime curvature and electromagnetic fields interact and influence each other.
Aliases (2)
Statements (51)
| Predicate | Object |
|---|---|
| instanceOf |
equations of motion
→
field equations → system of partial differential equations → theory in theoretical physics → |
| appliesTo |
curved spacetime
→
spacetimes with charged matter → vacuum with electromagnetic fields → |
| assumes |
classical (non-quantum) fields
→
general covariance → minimal coupling between gravity and electromagnetism → |
| basedOn |
Einstein field equations
→
Maxwell equations → |
| describes |
coupling of gravity and electromagnetism
→
interaction between spacetime curvature and electromagnetic fields → |
| expressedAs |
G_{μν} = 8π T_{μν}^{(EM)} + 8π T_{μν}^{(matter)}
→
∇_{[α} F_{βγ]} = 0 → ∇_{μ} F^{μν} = 4π J^{ν} → |
| field |
classical electromagnetism
→
general relativity → gravitational physics → relativistic field theory → |
| formulatedIn |
differential geometry
→
tensor calculus → |
| hasPart |
Einstein field equations with electromagnetic stress–energy tensor
→
Maxwell equations with covariant derivatives → source-free Maxwell equations in curved spacetime → |
| involvesQuantity |
Ricci curvature tensor R_{μν}
→
current four-vector J^{μ} → electromagnetic field tensor F_{μν} → electromagnetic stress–energy tensor T_{μν}^{(EM)} → metric tensor g_{μν} → scalar curvature R → |
| relatedTo |
Einstein equations
→
Einstein–Yang–Mills equations → Kaluza–Klein theory → Maxwell equations → classical field theory → |
| satisfies |
Bianchi identities through Einstein tensor
→
local charge conservation → |
| usedFor |
Kerr–Newman solution
→
Reissner–Nordström solution → electrovacuum solutions → modeling charged black holes → relativistic stellar models with charge → studying gravitational waves with electromagnetic fields → |
| uses |
Einstein tensor
→
Levi-Civita connection → Lorentzian metric → covariant derivative → electromagnetic field tensor → stress–energy tensor → |
Referenced by (4)
| Subject (surface form when different) | Predicate |
|---|---|
|
Israel–Carter–Robinson uniqueness theorems
("Einstein–Maxwell theory")
→
|
assumes |
|
Einstein–Maxwell equations
("Einstein field equations with electromagnetic stress–energy tensor")
→
|
hasPart |
|
Kerr–Newman black hole
→
|
solutionOf |
|
Reissner–Nordström metric
→
|
solves |