Lecture 21: General Relativity

Readings: Section 24-2

 

Key Ideas:

Postulates:

         Gravitational mass=inertial mass (aka Galileo was right)

         Laws of physics are the same for all observers

Consequences:

         Matter tells spacetime how to curve.

         Curved spacetime tells matter how to move.

         Clocks run more slowly in strong gravitational fields

Tests of General Relativity

         Perihelion Precession of Mercury

         Bending of light near the Sun/Galaxy Clusters

         Gravitational Redshift

         Gravity Waves

Relevance

General Relativity must be used for strong gravitational fields or for large accelerations

General Relativity is not a quantum theory and does not work on the smallest scales.

 

Newtonian Gravity

Matter tells gravitation how to exert a Force.

Forces tell matter how to accelerate.

 

A mass m is accelerated by the gravity of another mass M:

 

The acceleration due to gravity does not depend on the mass of the object being accelerated.

See nssdc.gsfc.nasa.gov/planetary/luna/Apollo_15_feather_drop.html for the video of an astronaut illustrating this point by dropping a feather and a hammer on the moon.

 

ÒI frame no hypothesisÓ

Newton could not explain what gravity was.

         He asserted that Gravity was an Òaction at a distanceÓ

He had no hypothesis for what ÒagentÓ communicates the gravitational force across empty space.

 

People assumed gravity worked as described, but didnÕt worry about whyÉ.

 

General Relativity

New way of looking at gravity. Maybe the motions of masses under gravity didnÕt have anything to do with the objects themselves.

 

Instead: Curved spacetime tells matter how to move.

Consequences:

         Photons affected by curved spacetime.

         Disagreement with the inverse square law (NewtonÕs Law of Gravity)

         Matter tells spacetime how to curve.

 

How do objects move in curved spacetime?

In flat space, they move in straight lines

Straight line=shortest distance between two points

 

The Shortest PathÉ

On a flat surface:

         The shortest path between two points is a straight line.

         Parallel lines stay parallel forever

On a curved surface:

         The shortest path is a curved line

Lines that start parallel can converge or diverge at some distance away.

 

A New Theory of Gravity

General Relativity may be summarized as:

         Matter tells spacetime how to curve.

         Curved spacetime tells matter how to move.

Replaces the Newtonian idea of a ÒforceÓ with the curvature of spacetime as the agent of Gravity.

 

GR has withstood all experimental tests.

 

The Laws of Physics are the same for all observers

NewtonÕs First Law:

Objects in motion will remain in motion in a straight line unless acted upon by an outside force.

General Relativity

Objects follow the shortest path in spacetime.

 

Final note: gravity same idea as acceleration (think roller coaster)

 

Tests of General Relativity

 

The Precessing Orbit of Mercury:

The major axis of MercuryÕs orbit precesses slowly by 574 arcseconds/century.

 

Einstein 1, Newton 0

 

Newtonian Gravity:

         Predicts precession of 531 arcsec/century

         ~43 arcsec/century smaller than observed

General Relativity

Spacetime curvature changes as Mercury gets closer to the sun on its orbit

Gives the orbit a little twist

This adds an extra 43 arcsec/century!!

 

Bending of Starlight

Light travels on the shortest path through spacetime.

Predication

         Gravity bends light passing a massive object

Confirmed:

         1919 Solar Eclipse

         Gravitational Lenses (1980s)

 

 

 

Einstein 2, Newton 0

 

Newtonian Gravity:

         Photons are massless and should not be bent by gravity.

General Relativity:

         Photons must also follow the shortest path in spacetime.

 

Gravitational Lens

Large clusters of galaxies have enough mass to ÒlensÓ the light of galaxies that lie behind them.

 

Example of Gravitational Lens

 

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Gravitational Redshift

 

Gravitational field affects time.

Clocks in stronger gravitational fields run slow.

If true, predicts a gravitational redshift

 

Wavelength of light seen from strong gravitational fields is redshifted.

(Note: different from Doppler shift)

 

Gravitational Redshift Observed

Pound & Rebka (1960) -- Harvard Tower

Hafele & Keating (1971) – jetlagged clocks

Scout D rocket (1976) – clocks on rockets

 

Gravitational Waves

Newton thought the force of gravity was instantaneously transported through space.

But, remember, in special relativity, information travels at the speed of light.

Changes in gravity are transmitted at the speed of light.

Gravity waves

         Travel at the speed of light

         Carry energy away

 

Binary Pulsar

2 pulsars=rapidly rotating neutron stars sending out radio jets

Accurate timing

Strong gravitational field

Test of theory

See system losing energy

         Pulsars are getting closer together

         75 millionths of a second/year different in period of pulses

Nobel Prize of Hulse & Taylor

 

Practical Relativity

Global Positioning System (GPS)

         24 satellites in high Earth orbit

         20,000 km altitude, 12h period (14,000 km/h)

         Carry on-board atomic clocks

Relativistic effects on these clocks

         Special Relativity 7 microseconds/day slower

         General Relativity 45 microseconds/day faster

Combined correction 45-7=38 microseconds/day

 

Whither Newton?

NewtonÕs laws are approximations of GR.

Conditions:

         Weak gravitational fields

         Speeds much slower than the speed of light

NewtonÕs Laws:

         Work accurately in the ÒeverydayÓ world.

         Are mathematically much simpler.

 

Status of General Relativity

It has passed every test weÕve thrown at it.

We will continue to test it, particularly in the strongest gravitational fields we can find.

Its effects must be included in binary pulsar calculations, collapses of stars to black holes, and in cosmology, among other applications.

Probably not the last word in gravity. We need a theory of quantum gravity.