The Mathematics of General Relativity, Black holes, and Cosmology Chad A. Middleton Brown Bag Seminar Mesa State College February 12, 2010.

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Presentation transcript:

The Mathematics of General Relativity, Black holes, and Cosmology Chad A. Middleton Brown Bag Seminar Mesa State College February 12, 2010

The Mathematics of General Relativity, Black holes, and Cosmology (in a Nutshell) Chad A. Middleton Brown Bag Seminar Mesa State College February 12, 2010

Galileo Galilei ALL objects fall at the same rate!

Newton’s Universal Law of Gravitation Successes Described the motion of massive bodies… …on earth …in the heavens

“Action at a distance”? Infinite propagation speed? Mercury’s perihelion precession? Shortcomings…

3D Euclidean Space Interval Line element in Euclidean space is the line element measuring length is invariant under rotations

In 1905, Einstein’s Theory of Special Relativity..  Lorentz Transformations  Length depends on reference frame

4D Spacetime Interval Line element in Minkowski (flat) spacetime is the line element measuring ‘length’ is invariant under ‘rotations’

Principle of Equivalence The motion of freely falling particles is the same in a gravitational field and a uniformly accelerated frame, in small enough regions of spacetime

Principle of Equivalence What about massless particles? Elevator observer sees light moving in a curved path! Spacetime is curved!

Line element in 4D curved space  is the metric tensor  encodes the geometry of spacetime  Know, know geometry

In 1915, Einstein’s gives the world his Theory of General Relativity describes the curvature of spacetime describes the matter & energy

When forced to summarize the general theory of relativity in one sentence; time and space and gravity have no separate existence from matter - Albert Einstein Matter tells space how to curve Space tells matter how to move

Einstein field equations  Subscripts label elements of each tensor  metric ( ) encodes the geometry of spacetime  A system of coupled, second-order, non-linear, differential equations

In 1916, Karl Schwarzschild presented an EXACT solution!  The line element for a static, spherically-symmetric massive object  Plug metric ansatz into the Einstein field equations in vacuum

The Einstein field equations become.. These coupled, non-linear, ODEs determine the line element exterior to a spherically-symmetric source

The empty space, spherically-symmetric, solution (i.e. spherical star) is described by Let: Notice: : Coordinate singularity : Spacetime singularity

Black Holes  For fixed radius R …  For M star > 3-4 M sun, star must collapse to a Black Hole Notice: Black Holes don’t suck! (External geometry of a Black Hole is the same as that of a star or planet)

Cosmology is the scientific study of the large scale properties of the Universe as a whole. addresses questions like: Is the Universe (in)finite in spatial extent? Is the Universe (in)finite in temporal extent? What are the possible geometries of the Universe? What is the fate of the Universe?

Friedmann-Robertson-Walker (FRW) Cosmology The line element for a spatially homogeneous, isotropic Universe evolving in time. Plug metric ansatz into the Einstein field equations for matter/energy modeled by a perfect fluid

The Einstein field equations become.. The density (  ), pressure (p), and curvature ( κ ) of the Universe determine the evolution of the scale factor (a)

Setting the spatial curvature to zero.. The density (  ) and pressure (p) of the Universe determine the evolution of the scale factor (a) These non-linear, ODEs determine the line element of a flat, homogeneous, isotropic spacetime

Choose an “equation of state” For radiation: For pressure-less matter: For a vacuum energy:

Density as a function of the scale factor Radiation dominated: Matter dominated: Vacuum energy dominated:

Conclusion General Relativity predicts…  the ultimate collapse of sufficiently massive stars to Black Holes GR & observational evidence indicate that:  the Universe is infinite in spatial extent  the Universe began w/ a “Big Bang” ~ 13.7 billion years ago  the Universe is flat  the Universe will continue to expand indefinitely

In 1929, Edwin Hubble discovered that the universe is expanding… What is the fate of the “decelerating” Universe?  “Big Crunch”  “Big Freeze”  Neither?

Recent Data from Type Ia Supernovae, WMAP and SDSS implies…  The Universe is flat  The expansion of the Universe is ACCELERATING!! The expansion of the Universe is ACCELERATING!!  Seems to imply a new form of Energy

Doppler Shift allows for determining the velocity of approaching/receding galaxies!

Cosmological Principle On sufficiently large distance scales, the Universe is 1. Isotropic 2. Homogeneous  Maximally Symmetric Space

For a Homogeneous & Isotropic Universe… … 3 possible Geometries Recent data indicates that the Universe is flat

Data from Type Ia Supernovae, WMAP and SDSS implies…  The Universe is flat  The expansion of the The expansion of the Universe is ACCELERATING!  Seems to indicate a Vacuum Energy

Georges Lemaître suggests the Universe had a temporal beginning.. Belgian Astrophysicist/ Catholic Priest 1927 paper in Annals of the Brussels Scientific Society Lemaître… showed that the universe had to be either contracting or expanding. suggested that the Universe had a definite beginning in which all its matter and energy were concentrated at one point.

Did the Universe begin with a “ Big Bang ”??  is not an explosion that happened at one point in space Big Bang - a time of infinite density, infinite temperature, and infinite spacetime curvature The “Big Bang”...  occurred at every place in one moment in time

In the early 1960’s, the Princeton group in gravitational physics… finds that the Universe should be uniformly bathed in a background microwave radiation predicts a blackbody spectrum of the background radiation w/ T ~ 10K

In 1965, observational evidence for the Big Bang!! Arno Penzias & Robert Wilson Bell Lab Physicists calibrating the Bell Labs microwave antenna designed for satellite communications Awarded the 1978 Nobel Prize in physics for discovery of the Cosmic Microwave Background Radiation

Yeah, but does this microwave background radiation have a Blackbody Spectrum? In Nov ‘89, NASA launches the Cosmic Background Explorer (COBE) to measure… the spectrum the anisotropies of the cosmic background radiation.

Spectrum of the Cosmic Microwave Background Radiation The excellent agreement with Planck’s law is the best fit ever measured! John Mather & George Smoot Awarded the 2006 Nobel Prize in physics “for their discovery of the blackbody form and anisotropy discovery of the CMB”

COBE image of the Cosmic Microwave Background Radiation Light from when the Universe was 380,000 years old… Map of  K anisotropies