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Dark energy - History |  | Dark energy - History: Encyclopedia II - Dark energy - History |  | The cosmological constant was first proposed by Einstein as a mechanism to obtain a stable solution of the gravitational field equation that would lead to a static universe, effectively using dark energy to balance gravity. Not only was the mechanism an inelegant example of fine-tuning, it was soon realized that Einstein's static universe would actually be unstable because local inhomogeneities would ultimately lead to either the runaway expansion or contraction of the universe. The equilibrium is unstable: if the universe expands slightly, ...
See also:Dark energy, Dark energy - Evidence for dark energy, Dark energy - Nature of dark energy, Dark energy - Cosmological constant, Dark energy - Quintessence, Dark energy - Other ideas, Dark energy - Implications for the fate of the universe, Dark energy - History |  | | Dark energy, Dark energy - Cosmological constant, Dark energy - Evidence for dark energy, Dark energy - History, Dark energy - Implications for the fate of the universe, Dark energy - Nature of dark energy, Dark energy - Other ideas, Dark energy - Quintessence, Dark-energy star |  | |
|  |  | Dark energy: Encyclopedia II - Dark energy - History
Dark energy - History
The cosmological constant was first proposed by Einstein as a mechanism to obtain a stable solution of the gravitational field equation that would lead to a static universe, effectively using dark energy to balance gravity. Not only was the mechanism an inelegant example of fine-tuning, it was soon realized that Einstein's static universe would actually be unstable because local inhomogeneities would ultimately lead to either the runaway expansion or contraction of the universe. The equilibrium is unstable: if the universe expands slightly, then the expansion releases vacuum energy, which causes yet more expansion. Likewise, a universe which contracts slightly will continue contracting. These sorts of disturbances are inevitable, due to the uneven distribution of matter throughout the universe. More importantly, observations made by Edwin Hubble showed that the universe appears to be expanding and not static at all. Einstein famously referred to his failure to predict the idea of a dynamic universe, in contrast to a static universe, as his greatest blunder. Following this realization, the cosmological constant was largely ignored as a historical curiosity.
Alan Guth proposed in the 1970s that a negative pressure field, similar in concept to dark energy, could drive cosmic inflation in the very early universe. Inflation postulates that some repulsive force, qualitatively similar to dark energy, resulted in an enormous and exponential expansion of the universe slightly after the Big Bang. Such expansion is an essential feature of most current models of the Big Bang. However, inflation must have occurred at a much higher energy density than the dark energy we observe today and is believed to have completely ended when the universe was just a fraction of a second old. It is unclear what relation, if any, exists between dark energy and inflation. Even after inflationary models became accepted, the cosmological constant was believed to be irrelevant to the current universe.
By 1998, the missing mass problem of big bang nucleosynthesis and large scale structure was established, and some cosmologists had started to theorize that there was an additional component to our universe, with properties very similar to dark energy. This suspicion was reinforced by supernova observations of accelerated expansion, simultaneously released by the teams of Riess et al and Perlmutter et al. This resulted in the Lambda-CDM model, which as of 2005 has remained consistent with a series of increasingly rigorous cosmological observations, the latest being the 2005 Supernova Legacy Survey. [1]
Other related archives1970s, 1990s, 1998, 2005, Age of the universe, Alan Guth, Astrophysics, Big Bang, Big Crunch, Big Rip, Chandrasekhar limit, Comoving distance, Compton wavelength, Cosmic microwave background, Dark matter, Dark-energy star, Earth, Edwin Hubble, Einstein, FLRW metric, Friedmann equations, Galaxy formation, General relativity, Hubble's law, Inflation, Lambda-CDM model, Large-scale structure, Michael Turner, Milky Way, Nucleosynthesis, Observable universe, Particle physics, Perlmutter, Quantum gravity, Redshift, Scalar fields, Shape of the universe, Steven Weinberg, Timeline of cosmology, Timeline of the Big Bang, Ultimate fate of the universe, Universe, Virgo supercluster, WMAP, absolute magnitude, anthropic principle, apparent magnitude, baryons, big bang nucleosynthesis, brane cosmology, cosmic horizon, cosmic inflation, cosmic microwave background, cosmological constant, cosmology, critical density, cyclic model, dark matter, dense, dynamical, economical solution, electrical, energy, energy scale, equation of state, equation of state (cosmology), equilibrium, equivalence principle, field, fine-tuning, flat, fundamental forces, galaxies, galaxy clusters, general relativity, gravitational field equation, gravitational lensing, gravity, heat death, holographic principle, homogeneous, kinetic energy, large scale structure, local supercluster, matter-radiation equality, missing mass, negative pressure, nuclear forces, orders of magnitude, particle physics, phantom energy, problem, quantum field theories, quasars, quintessence, redshift, reduced Planck units, renormalization, shape of the universe, solar system, special relativity, standard candles, standard model, stars, string theory, structure, superclusters, supersymmetric, theory of relativity, type Ia supernovae, universe, vacuum, vacuum energy, vacuum fluctuations, variation of the fundamental constants, white dwarf
 Adapted from the Wikipedia article "History", under the G.N U Free Docmentation License. Please also see http://en.wikipedia.org/wiki |
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