Friedmann equations
The Friedmann equations are a set of equations in physical cosmology that govern the expansion of space in homogeneous and isotropic models of the universe within the context of general relativity. They were first derived by Alexander Friedmann in 1922 from Einstein's field equations of gravitation for the Friedmann–Lemaître–Robertson–Walker metric and a perfect fluid with a given mass density ? {\displaystyle \!\rho } and pressure p {\displaystyle \!p}. The equations for negative spatial curvature were given by Friedmann in 1924.
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Friedmann equations
The Friedmann equations are a set of equations in physical cosmology that govern the expansion of space in homogeneous and isotropic models of the universe within the context of general relativity. They were first derived by Alexander Friedmann in 1922 from Einstein's field equations of gravitation for the Friedmann–Lemaître–Robertson–Walker metric and a perfect fluid with a given mass density ? {\displaystyle \!\rho } and pressure p {\displaystyle \!p}. The equations for negative spatial curvature were given by Friedmann in 1924.
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Overview

The Friedmann equations are a set of equations in physical cosmology that govern the expansion of space in homogeneous and isotropic models of the universe within the context of general relativity. They were first derived by Alexander Friedmann in 1922 from Einstein's field equations of gravitation for the Friedmann–Lemaître–Robertson–Walker metric and a perfect fluid with a given mass density ? {\displaystyle \!\rho } and pressure p {\displaystyle \!p}. The equations for negative spatial curvature were given by Friedmann in 1924.

Product Details

BN ID: 2940156739813
Publisher: Euprint press Limited
Publication date: 07/18/2016
Sold by: Barnes & Noble
Format: eBook
File size: 164 KB
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