Lecture 20 Professor Stephen Thornton April 11,...

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PHYS 202 Lecture 20 Professor Stephen Thornton April 11, 2006

Transcript of Lecture 20 Professor Stephen Thornton April 11,...

Page 1: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

PHYS 202

Lecture 20Professor Stephen Thornton

April 11, 2006

Page 2: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Reading Quiz

Black holes

1) are imaginary objects, because they cannot be detected.

2) are objects that absorb all light and then emit light over all wavelengths.

3) can be inferred by the effects they exert on neighboring bodies.

4) are made by the “black death” plague ofthe middle ages.

Page 3: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Answer: 3Black holes absorb all light that reaches them. They do not emit light. They can only be indirectly observed by effects they cause on neighboring bodies – for example, by a neutron star rotating around a black hole.

Page 4: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Last time – started relativityUp to 1895Special relativityTime dilationTwin agingLength contractionRelativistic addition of velocities

Page 5: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Today

Relativistic momentum, mass, energy.Einstein mass-energy relation.AntimatterPETGeneral relativity – bending of lightSpacetime warp, black holes

Page 6: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Conceptual Quiz:Will the stick simultaneously fit into the manhole? Which possibility is correct?

1) Possibility 12) Possibility 23) The stick will not fit into

the hole.

Page 7: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

According to Postulate 1 all laws of physics are the same in all inertial frames of reference.

The conservations of linear momentum and energy are still valid.

Momentum will appear different.

2 2***

1 /mvp mvv c

γ= =−

2 2

11 /v c

γ =−

Page 8: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Relativistic Momentum

Remember 1%-5%

Page 9: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

There is some controversy as to whether we can write p = mv and consider a relativistic mass m = γ m0. Most physicists, and I am one of them, do not subscribe to the concept that mass increases with velocity.

Mass is an invariant quantity and has the same mass m = m0 irrespective of speed.

We will simply have different equations for momentum and energy. p mvγ=

Page 10: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Energy

0

20

2rest 0 0

2 2 2total rest 0 0 0

If we use calculus, we find

( )

We still use the work-energy theorem to relatekinetic energy and work.

( 1)

Rest energy (or simply )

( 1)

dp dF m vdt dt

K m c

E m c E

E K E m c m c m c

γ

γ

γ γ

= =

= −

= + = − + =

Page 11: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Famous Einstein relation2

rest 0

2total 0

E m c

E m cγ

=

=

Sun

Page 12: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

What happens when we squeeze the spring?

The best explanation is to say that the energy increases. E = m0c2 because K = 0. In this case we would say the rest mass m0increases. It does so because of energy, not because it is moving.

Page 13: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

We also have a relation between energy and momentum. A careful comparison shows

2 2 2 2 40

0

***Note that for light, 0,and .

E p c m cm

E pc

= +

=

=

Page 14: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Work Problems 29-3629-4829-59

Page 15: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Conceptual QuizThe mass of a cup of steaming Starbucks coffee is

1) larger2) smaller3) the same4) no way to know

than it is when cold.

Page 16: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Answer: 1

Because of the famous Einstein energy relation, E = mc2, the mass of the hot cup of coffee is greater.

Page 17: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Conceptual Quiz:Consider an electron moving at a speed of v = 105 m/s. The rest mass of an electron is m0. Which of the following answers most correctly describes the kinetic energy of the electron to within 1% accuracy?

1) m0v2/22) m0c2(γ - 1) 3) Both equations work. 4) Neither equation works.5) Not enough information is given.

Page 18: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Answer: 3

An electron with speed v = 105 m/s is so much smaller than c that we can use either equation because γ = 1.000006.

Generally v/c ≈ 0.05 before we need to use relativistic results.

Page 19: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Electron–Positron Annihilation

What is antimatter?

Page 20: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Positron emission tomographyA radioactive chemical containing a positron emitter (e+) like 15O, 11C, 13N, 18F is injected into the body to study a particular object.

Page 21: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

PET scans

Page 22: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Proton-antiproton interaction

The most efficient form of energy conversion known is for antimatter.

Dan Brown’s Angels and Demons discusses antimatter bomb that will destroy the Vatican. Watch out for the Illuminati!

Page 23: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Top: gravityBottom: acceleration

Person in enclosure cannot tell whether gravity or acceleration is acting on them and the ball.

Principle of Equivalence:All physical experiments conducted in a uniform gravitational field and in an accelerated frame of reference give identical results.

Page 24: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Light pulse in elevator.

As elevator moves up, light pulse goes down.

Page 25: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

A Light Experiment in Two Different Frames of Reference

Page 26: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

The Principle of Equivalence

Einstein proved that light must be bent in a gravitational field.

Page 27: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

General RelativityAlbert Einstein published his special theory of relativity in 1905 while a patent clerk in Bern, Switzerland.

He published his general theory of relativity in 1916. How could it be proven?

Page 28: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Gravitational Bending of LightNormally we cannot see positions of stars near the sun to see if they are apparently moved, but during an eclipse by the moon, we can. Fortunately, there was an eclipse in 1919 in the southern hemisphere.

Page 29: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Bending of Light Near the Sun

Eddington mounted expeditions to Africa and South America in 1919 to attempt to prove whether Einstein was correct. A few months later, Einstein was the world’s best known scientist. It is said that only a handful of physicists actually understand the general theory of relativity.

Page 30: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Einstein cross

Page 31: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Schwarzchild radiusE

E

2

2 escape speed from Earth

Body of mass and radius :

2

2

No light inside this radius can leave the body

e

e

GMvR

M R

GMv cR

GMRc

=

= =

=

BLACK HOLE!!

Page 32: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Black hole evidence

Prediction

Actual Hubble image of M87 galaxy

Page 33: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Warped Space and Black Holes

Light rays are bent near gravity.

Warped space!

Black holes can do this.

Page 34: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

A neutron star orbiting a black hole can emit gravity waves.

Page 35: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Laser Interferometer Gravitational Wave ObservatoryHow LIGO Detects a Gravity Wave

Page 36: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

LISA – ESA and NASA

Planned for launch in 2011. Three satellites will be in space to detect gravity waves.

Page 37: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Gravity Probe B – launched April 2004Gravity Probe B is a relativity gyroscope experiment to test two extraordinary, unverified predictions of Albert Einstein's general theory of relativity.

1) The curved spacetime, or geodetic, effect- Einstein's theory predicted that the presence of a mass in space, such as the Earth, would warp local spacetime, creating a dip or curve in spacetime.

2) The frame-dragging effect- A few years after Einstein published his theory, physicists Lense and Thirring predicted that the rotation of a mass in space would twist or drag the local spacetime frame around it.

To observe and measure these effects, Gravity Probe B launched four sophisticated gyroscopes into low-Earth polar orbit(400 miles) in April 2004. After calibration, it took data for almost a year until June 2005. No results have yet been reported. Whilein orbit, each gyroscope's spin axis was monitored as it traveled through local spacetime.

Page 38: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Work Problem 29-73

Page 39: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Conceptual Quiz:The theory of relativity limits the maximum speed that an object can have. Is there a similar restriction on the maximum energy or momentum?

1) no for both2) yes for energy, no for momentum3) no for energy, yes for momentum4) yes for both

Page 40: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Answer: 1

There is no restriction on either.

Page 41: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Conceptual Quiz:We observe a clock in a moving rocket runing slow. What happens to the clock if the rocket reverses direction and moves with the same speed.

1) clock still runs slow.2) clock runs fast.3) clock is normal.

Page 42: Lecture 20 Professor Stephen Thornton April 11, 2006galileo.phys.virginia.edu/classes/202.stt.spring06/Thornton Lecture... · Relativistic addition of velocities. Today Relativistic

Answer: 1Clock still runs slow.