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From Special to General Relativity

Manual: General · Subject: Physics

Transitions from inertial frames to curved spacetime, equivalence principle, and gravitational physics.

Beyond Inertial Frames

Equivalence Principle

Einstein’s equivalence principle states that locally, gravitational effects are indistinguishable from acceleration. This suggests that gravity is not a conventional force in spacetime, but rather a manifestation of spacetime geometry.

Curved Spacetime

General relativity replaces the Minkowski metric with a dynamical metric gμν(x)g_{\mu\nu}(x). In curved spacetime, proper intervals are given by ds2=gμνdxμdxν,ds^2 = g_{\mu\nu}dx^\mu dx^\nu, and free-fall trajectories are geodesics.

Local vs Global Inertial Structure

Special relativity remains valid locally in freely falling frames, but no single global inertial frame exists in a generic gravitational field. Tidal effects reveal curvature through relative accelerations.

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Conceptual Bridge

The move from SR to GR is the move from flat geometry with global inertial symmetry to dynamical geometry with local Lorentz symmetry.

What is the strongest motivation for general relativity from the equivalence principle?

What mathematical object becomes dynamical in general relativity?

SR and GR

FeatureSpecial RelativityGeneral Relativity
Spacetime geometryFlat MinkowskiCurved and dynamical
SymmetryGlobal Lorentz invarianceLocal Lorentz invariance
GravityAbsentGeometrized
Free motionStraight worldlinesGeodesics

What reveals spacetime curvature physically?

Conceptual Progression to GR

  1. 1

    Step 1: Recognize the local validity of SR.

  2. 2

    Step 2: Apply the equivalence principle to accelerated frames.

  3. 3

    Step 3: Promote the metric to a gravitational field.

  4. 4

    Step 4: Describe gravity through geodesics and curvature.