fomalhaut b and newton's general solution to kepler's third law

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Fomalhaut B and Newton’s General Solution To Kepler’s Third Law Professor Madigan

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The first direct observation of an exoplanet in orbit around its parent star was made by the Hubble Space Telescope. The observation is used to demonstrate the universal application and veracity of Newton's Universal Law of Gravitation, his general solution to Kepler's Third Law and Kepler's first 2 laws and that gravitation is the underlying driving principle behind it all.

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Page 1: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut Band

Newton’s General Solution To

Kepler’s Third Law

Professor Madigan

Page 2: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut

Page 3: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut is only 25 light years distant, is the

brightest star in Piscis Australis, The Southern

Fish and is visible during the late summer

Fomalhaut is twice the mass of the sun, over 17

times its luminosity and a productive life span of

only 10% of the sun’s

Results published in March of 2009 by Paul Kalas

and Eugene Chiang of UC, Berkeley show that

Fomalhaut B is the first exoplanet directly

imaged and orbit around its host star confirmed

by direct observation

Page 4: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut is only 25 light years distant; is the brightest star in Piscis Australis, The Southern Fish, and is visible during late summer

Fomalhaut is twice the mass of the sun and over 17 times its luminosity

Results published in March of 2009 by Paul Kalas and Eugene Chiang of UC, Berkeley show that

Fomalhaut B is the first exoplanet directly

imaged and orbit around its host star

confirmed by direct observation

Page 5: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut is only 25 light years distant; is the

brightest star in Piscis Australis, The Southern

Fish, and is visible during late summer

Fomalhaut is twice the mass of the sun, over 17

times its luminosity and a productive life span of

only 10% of the sun’s

Results published in March of 2009 by Paul Kalas

and Eugene Chiang of UC, Berkeley show that

Fomalhaut B is the first exoplanet directly

imaged and orbit around its host star confirmed

by direct observation

Page 6: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut is only 25 light years distant; is the

brightest star in Piscis Australis, The Southern

Fish, and is visible during late summer

Fomalhaut is twice the mass of the sun, over 17

times its luminosity and a productive life span of

only 10% of the sun’s

A study published in March 2009 by Paul Kalas

and Eugene Chiang of the University of

California, Berkeley:

Fomalhaut B is the first exoplanet directly imaged

whose orbit around its host star is confirmed by

direct observation

Page 7: Fomalhaut B and Newton's General Solution to Kepler's Third law

Fomalhaut is only 25 light years distant; is the

brightest star in Piscis Australis, The Southern

Fish, and is visible during late summer

Fomalhaut is twice the mass of the sun, over 17

times its luminosity and a productive life span of

only 10% of the sun’s

A study published in March 2009 by Paul Kalas

and Eugene Chiang of the University of

California, Berkeley:

Fomalhaut B is the first exoplanet directly imaged

whose orbit around its host star is confirmed by

direct observation

Page 8: Fomalhaut B and Newton's General Solution to Kepler's Third law
Page 9: Fomalhaut B and Newton's General Solution to Kepler's Third law
Page 10: Fomalhaut B and Newton's General Solution to Kepler's Third law
Page 11: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical.

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 12: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 13: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 14: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 15: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 16: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 17: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 18: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 19: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 20: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 21: Fomalhaut B and Newton's General Solution to Kepler's Third law

A quick review of Kepler’s laws1. All orbits are elliptical

Why?

Gravitation

2. Equal areas in equal times

Why?

Gravitation

3. The orbital period of any body in orbit about

another varies as the 3/2 power of its semimajor

axis

Why?

Gravitation

These laws are universally applicable and are not

restricted to any system

Page 22: Fomalhaut B and Newton's General Solution to Kepler's Third law

Using the Hubble Space Telescope,

Fomalhaut B was directly

imaged and its orbit empirically

measured over a 2 year period

Page 23: Fomalhaut B and Newton's General Solution to Kepler's Third law
Page 24: Fomalhaut B and Newton's General Solution to Kepler's Third law

We thus certify the veracity of all

Kepler’s Laws and their

inexorable link to gravity as the

universal driving principal and

the generality of Newton’s

Universal Law of Gravitation

Page 25: Fomalhaut B and Newton's General Solution to Kepler's Third law

We choose Kepler’s 3rd law and,

using Newton’s original

derivation, provide an

empirically demonstrable

solution for Fomalhaut B’s

orbital characteristics

Page 26: Fomalhaut B and Newton's General Solution to Kepler's Third law

2

31

P

A

2 3P A

Page 27: Fomalhaut B and Newton's General Solution to Kepler's Third law

What is the significance of the

“1” in this expression?

Page 28: Fomalhaut B and Newton's General Solution to Kepler's Third law

It represents the total mass of the

system

Page 29: Fomalhaut B and Newton's General Solution to Kepler's Third law

2

( )3 Tot

PM

A

In terms of Solar Masses and Earth

Years, we find:

Page 30: Fomalhaut B and Newton's General Solution to Kepler's Third law

2 3

( )TotP A M

Page 31: Fomalhaut B and Newton's General Solution to Kepler's Third law

3

( )TotP A M

Page 32: Fomalhaut B and Newton's General Solution to Kepler's Third law

Using the empirically determined

distance of 115 AU from Fomalhaut

to Fomalhaut B, we compute the

period of Fomalhaut B to be:

3(115) 2

11744 872

2

P x

SolarMassP x yrs

Page 33: Fomalhaut B and Newton's General Solution to Kepler's Third law

Deriving Newton’s General Form for

Kepler’s Third Law, equating the force

of gravity of the two bodies to the

centripetal force of the planet in orbit

around the center of mass, we find:

1 2( ) 2

2

2( )

2

1 2 2

2

G

Cent

M MF G

a

M vF

a

M M M vG

a a

Page 34: Fomalhaut B and Newton's General Solution to Kepler's Third law

22 2

1

2 2

2

1

2 2

2

1

3 2

3 2

1 2

1 2 4

4

4

4

M v a aG

a a a p p

M aG

a p

MG

a p

aGM

p

Page 35: Fomalhaut B and Newton's General Solution to Kepler's Third law

3 2

1 2

4aGM

p

Newton’s General Form

Of

Kepler’s 3rd Law

Page 36: Fomalhaut B and Newton's General Solution to Kepler's Third law

Solving this general equation for the

period, we find:

2 310

1

10

7 1

42.751 10 sec

2.751 10 sec872

3.156 10 sec

aP x

GM

xyrs

x yr

Page 37: Fomalhaut B and Newton's General Solution to Kepler's Third law
Page 38: Fomalhaut B and Newton's General Solution to Kepler's Third law