the “fuel cycle” of the sun. last time: chemical reactions have far too little energy available...

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The “fuel cycle” of the Sun

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Page 1: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The “fuel cycle” of the Sun

Page 2: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Last time: chemical reactions have far too little energy available per mass to power

the Sun over geological time

Page 3: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Some vastly more powerful energy source (than chemical reactions) must

be occurring in the Sun and stars

Page 4: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

A microscopic view of chemical reactions: interactions of the electron cloud

Page 5: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Nuclear reactions: interactions among the nuclei (Figure 17.2)

Page 6: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Nuclear Reactions in Stellar Interiors

H + H

2H + e+ + nu

H + 2H 3He + gamma

3He + 3He 4He + H + H

Net effect: 4H 4He

Question: why does this occur exclusively in the core of a star?

Demo

Page 7: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

A small mass difference between Hydrogen and

Helium

• 4 Hydrogen atoms: 6.693E-27 kg

• 1 Helium atom: 6.645E-27 kg

• Difference = 0.048E-27 kg

• Difference = 0.7 percent

Why is this small difference important?

Page 8: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The Einstein Energy-Mass equivalence relation

E=mc2

c=speed of light

You get a lot of bang for the buck: 6.3E+14 J/kg

Page 9: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Stars have a lot of fuel in the form of hydrogen

These abundancesAre characteristic of the Solar photosphere, andNearly all other stars

Page 10: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The Power Source of Main Sequence Stars

MS stars fuse hydrogen into helium, releasing prodigious amounts of energy in the process. Their fuel source is the matter

of which they are made

Page 11: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The Structure of Main Sequence Stars

The Powerhouse

Page 12: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

How can we tell if this is right? Detect neutrinos emitted from

the center of the Sun.

Page 13: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The Neutrino Sun: A View into the Solar Interior

Page 14: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The fuel for a main sequence star is its own mass in the form of hydrogen.

The total amount of fuel is proportional to the total mass of the star.

What are the masses of stars?

Page 15: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

How We Determine Masses of Stars

Method:observation of binary stars (double stars)

Page 16: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Binary stars are numerous (e.g. Sirius)

Page 17: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

We can see orbital motion of Sirius B around Sirius A

Page 18: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

Masses of stars determine the gravitational force, and thus the

acceleration of the stars

Page 19: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

A little gravitational physics

If M >>m

V2 = GM/r

Or M=V2r/G

From observations of motions of binary stars, one can determine their masses

Page 20: The “fuel cycle” of the Sun. Last time: chemical reactions have far too little energy available per mass to power the Sun over geological time

The Types of Binary Stars

• Visual Binaries

• Eclipsing Binaries

• Spectroscopic Binaries