Physic Labs

Theory of relativity

The Einstein field equations

Explore a mesh of curvature illustrating the Einstein field equation Gμν=8πGc4TμνG_{\mu\nu}=\frac{8\pi G}{c^4}T_{\mu\nu}: regions of greater energy–stress density make the mesh sag deeper. Adjust the source strength and the time rate to compare the sag.

Research

Equipment

  • Virtual spacetime mesh showing sag caused by the source
  • Source-density slider (dimensionless parameter)
  • Time-speed slider and Pause button
  • Draggable canvas; source-parameter readout

Procedure

  1. Read the mesh sag

    Leave the source parameter at its middle value and press Pause. Drag the canvas to tilt the view and inspect the depth of the sag: the closer to the source, the deeper the mesh dips — a qualitative picture of Gμν=8πGc4TμνG_{\mu\nu}=\frac{8\pi G}{c^4}T_{\mu\nu}.

  2. Vary the source density

    Raise the source-density slider from low to high and note the 'source parameter' readout together with the relative sag. The larger TμνT_{\mu\nu}, the stronger the depicted curvature — the spirit of the linear relation Gμν∝TμνG_{\mu\nu}\propto T_{\mu\nu}.

  3. Compare vacuum-like conditions and predict

    Drop the source to its lowest setting: the region far from the source is nearly flat, recalling the vacuum solution Rμν=0R_{\mu\nu}=0 outside a mass. Use the time-speed slider to change the animation pace, predict the sag for a doubled source, then check.

Simulation

Experiment history

Albert Einstein presented the final field equations to the Prussian Academy of Sciences on 25 November 1915, after years of seeking a relativistic theory of gravity; that same month Karl Schwarzschild found the first exact vacuum solution. Explaining Mercury's anomalous perihelion precession, and then the 1919 light-deflection measurements, established the theory. The equation Gμν+Λgμν=8πGc4TμνG_{\mu\nu}+\Lambda g_{\mu\nu}=\frac{8\pi G}{c^4}T_{\mu\nu} states that energy and stress determine spacetime curvature, while curvature tells matter how to move. Einstein added the cosmological constant Λ\Lambda in 1917, later abandoned it, and it returned when 1990s observations showed the expansion of the universe accelerating.

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