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  1. Einstein’s Explanation of Photoelectric Effect. Einstein resolved this problem using Planck’s revolutionary idea that light was a particle. The energy carried by each particle of light (called quanta or photon) is dependent on the light’s frequency (ν) as shown: E = hν. Where h = Planck’s constant = 6.6261 × 10-34 Js.

  2. Jun 22, 2013 · Einstein's Field Equations for General Relativity - including the Metric Tensor, Christoffel symbols, Ricci Cuvature Tensor, Curvature Scalar, Stress Energy ...

    • 126 min
    • 4.5M
    • DrPhysicsA
  3. 3 Einstein’s Equation To state Einstein’s equation in simple English, we need to consider a round ball of test particles that are all initially at rest relative to each other. As we have seen, this is a sensible notion only in the limit where the ball is very small. If we start with such a ball of particles, it will, to second order in time ...

  4. The Einstein–Infeld–Hoffmann equations of motion, jointly derived by Albert Einstein, Leopold Infeld and Banesh Hoffmann, are the differential equations describing the approximate dynamics of a system of point-like masses due to their mutual gravitational interactions, including general relativistic effects. It uses a first-order post ...

  5. Description: The Einstein curvature tensor, a variation on the Ricci curvature, defined so that it has vanishing covariant divergence. Using this tensor, we at last build a field theory for spacetime, motivating the Einstein field equation by arguing how to generalize a gravitational field equation to relativity. Instructor: Prof. Scott Hughes.

  6. The Einstein field equations (EFE; also known as "Einstein's equations") are the set of ten equations in Albert Einstein's general theory of relativity that describes the fundamental interaction of gravitation as a result of spacetime being curved by matter and energy. [1] First published by Einstein in 1915 [2] as a tensor equation, the EFE ...

  7. The Einstein–Hilbert action—and the Einstein equations—can be viewed as having the simplest forms that do not ultimately depend on the choice of coordinates. Higher-order terms—say powers of the Ricci scalar curvature—could well arise from underlying network systems, but would not contribute noticeably except in very high gravitational fields.

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