Astro 1 - Lecture 16


Matthew A. Bershady

Department of Astronomy & Astrophysics

Penn State University


Fall 1996

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© 1995 Matthew A. Bershady

Lectures Lecture page Astro1 page



SOL




... a typical star, average in mass, composition, and luminosity ...


1. Solar structure:


Core

Interior

Convection zone

Photosphere - the solar disk - very thin

5800 degrees (K)

Chromosphere - lower atmosphere, where absorption lines are formed

(transition region)

Corona - upper atmosphere - very hot and tenuous

How is heated?

Energy from magnetic fields?

trends of temperature and density



2. Energy transport


radiation:

free streaming of photons or other energetic particles

convection:

overturning of cells of matter at different temperatures


Solar radiative zones:

most of the interior of the sun
Core
Interior
and, the Photosphere


Convective zones:

outermost layer of the interior before the photosphere

convective cells get smaller at larger radii

(cooler temperatures, lower densities)




3. Solar surface


Due to, or shaped by magnetic fields:

sunspots
slightly cooler regions of photosphere
300-1300 degrees (K) cooler
spicules
prominences
flares

Due to convection:

granules (granulation)
roughly 1000 km in size
super-granules (super-granulation)
roughly 30,000 km in size



4. Sunspot and Solar cycles


11 years - sunspot cycle (minimum and maximum activity)

22 years - solar cycle (orientation of magnetic fields)

Why?

differential rotation

twisting of field lines




5. Solar Guts - Fusion Revisited


Incredible energy production from: fusion +

(i) E = mc2

(ii) total matter and energy are always conserved


The proton-proton chain:

6 protons (6 H nuclei)
2 protons + 2 neutrinos + 2 positrons + He-4

where,

He-4 (Helium-4) = 2 protons + 2 neutrons

neutrinos: almost massless

positrons = anti-electrons

- weigh much less than proton or neutron

Add up input and output mass:

input mass > output mass

Energy MUST be released

Mass difference is primarily due to the difference in the mass of the proton and neutron (neutron is lighter )

mass(proton) > mass(neutron)




6. Solar neutrinos


- a disturbing puzzle

- where are they? (why don't we detect them?)

- neutrino oscillations?




7. Age of the Sun


Per fusion event (4 protons Helium) :

m = mass(proton) - mass(neutron)

2 x m = 4.8 x 10-29 kg

c2 = 9 x 1016 m2 /s2

E = mc2 = 2 x m c2 = 4.3 x 10-12 Joules (kg m2/s2)

lifetime = [total mass]
x [energy release per unit mass] / [energy radiated per sec]

radiant energy: 3.9 x 1026 Joules per s

total mass: 2 x 1030 kg

energy per unit mass: 6.4 x 1014 J per kg

lifetime: about 10 billion years




Q16.1 Which of the following does not occur -- at least in part -- in the Sun's photosphere:

(a) flares

(b) fusion

(c) sunspots

(d) radiation

(e) spicules

Q16.2 What is the key aspect of the proton-proton fusion chain reaction that produces energy to drive the Sun's radiation?

(a) mass and energy are convertible and conserved overall

(b) the neutrino can pass through light-years of lead

(c) fusion drives convection in the outer layers of the sun

(d) the mass of the protons are less than the resulting neutrons

(e) proton-proton interactions conserve angular and linear momentum


Lectures Lecture page Astro1 page

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Last updated: Sep 21, 1996 Matthew A. Bershady