Space and Astronomy Atlas

How The Universe Works
Sign In
Text size
100%
Theme
Concept

Cosmological Constant

Cosmology and the Early Universe

The cosmological constant is a term Albert Einstein added to his field equations of general relativity to represent the energy density of empty space, sometimes called vacuum energy. Einstein introduced it in 1917 to permit a static universe, then withdrew his support once the universe was shown to be expanding; the concept was later revived to help explain the observed accelerating expansion attributed to dark energy.

Facts
Concept Domain
Cosmology 1
Formulated Year
1917 1
Proposed By
Albert Einstein 1
Connections

Associated With

Source Wikipedia (space and spaceflight articles)
Dark Energy, Concepts
Source Wikipedia (space and spaceflight articles)
Dark Energy, Concepts
Source Wikipedia (space and spaceflight articles)
Multiverse, Concepts
In the Other Atlases

Originated In

Also in Science Atlas: where this subject originated.

Source Wikipedia (space and spaceflight articles)
Sources
1. Wikipedia (space and spaceflight articles)
Wikimedia Foundation
  • Cosmological constant, lead section
    a coefficient that Albert Einstein initially added to his field equations of general relativity to express the energy density of space, or vacuum energy
  • Associated With: Dark Energy
  • Associated With: Big Bang Theory
View the Source
Cosmological constant (Wikipedia)
  • Cosmological constant, history section
    Einstein introduced the constant in 1917 to counterbalance the effect of gravity and achieve a static universe, which was then assumed.
  • In Group: Dark Matter and Dark Energy, Lead sentence
    In physical cosmology, the cosmological constant (usually denoted by the Greek capital letter lambda: Λ), alternatively called Einstein's cosmological constant, is a coefficient that Albert Einstein initially added to his field equations of general relativity.
View the Source

Take a Related Quiz

Comments (0)
No comments yet. Be the first to share a thought.
Reader Challenges (0)
No disputes yet. Spotted an error or a better source? Open the first one.