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- Chapter Outline
- Why Does the Sun Shine?
- Plunging to the Center of the Sun: An Imaginary Journey
- The Cosmic Crucible
- From Core to Corona
- Solar Weather and Climate
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- The fundamental behavior of the natural world that we uncover in Earth
laboratories, such as expressed in conservation of energy and momentum,
are assumed universally applicable and have not been shown to be flawed
by any defensible study to date.
- By application of these fundamental laws in mathematical form, we can
compute theoretical stellar models as a means of studying internal
structure even though the deep interior is not directly accessible by
observation.
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- Life story of star
- Gravity squeezes, pressure forces resist by pushing out
- Energy loss in luminosity decreases pressure
- Energy generation replaces losses
- When energy generation stops star is dead
- Pressure forces
- Kinetic pressure of hot gases
- Electron degeneracy pressure from exclusion principle
- Neutron degeneracy pressure from exclusion principle
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- Perfect gas - solar gases almost totally ionized, behavior of nuclei and
free electrons is such that pressure is proportional to temperature and
density
- Hydrostatic equilibrium - weight of overlaying layers balanced by
pressure of hot gas pushing out
- Equation: weight of gas =
pressure of hot gas
- Results: star neither expands
nor contracts
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- Energy generation - energy source that replaces energy loss from
luminosity
- If Sun radiated only because it is hot, Sun would cool at measurable
rate
- Sun is not observed to be cooling
- Consequently, interior stays hot by releasing energy
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- Thermal equilibrium - amount of energy produced inside equals amount
radiated away as luminosity
- Solar gases obey perfect gas law, P
µ r T
- Self-regulating mechanism
- If too much energy produced, Sun heats up and expands
- If too little energy produced, Sun cools down and contracts
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- Thermonuclear fusion - fusion of small mass nuclei, primarily hydrogen
nuclei, to form more massive nuclei, primarily helium, with resulting
direct conversion of mass into energy by
- Einstein’s mass-energy equivalence:
E = mc2
- Equation: 41H1 Ţ 4He2 + g + n + e+
- where 1H1
= hydrogen nucleus, proton
- 4He2
= helium nucleus, 2 protons, 2 neutrons
- g = gamma-ray photons
- n = neutrinos
- e+
= positron
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- Energy transport - various physical processes transport energy from deep
interior to surface
- Radiative transport - energy moves outward by absorption and
re-emission by matter
- Energy generated as a few high-energy gamma-ray photons
- Absorption and re-emission degrades high-energy gamma-ray photons to low-energy
visible photons
- Opacity - resistance offered by matter to movement of radiation
- Convective transport - mass motions move energy
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- Solar model - mathematical model for study of structure and evolution of
the Sun and other stars
- Solar structure equations - describe variation of mass, pressure,
temperature, and luminosity from center to surface
- Mass conservation - total mass equals sum of masses for each layer
- Hydrostatic equilibrium - weight of overlying layer balanced by outward
pressure of hot gases
- Energy conservation - luminosity equals sum of energy generation in
each layer
- Energy transport - energy moves from hot (high-energy density) region
to cool (low-energy density) region
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- Equations solved for about 200 points along radius and for particular
time in the Sun’s life
- Result - solar model
- Confirms importance of various physical processes inside real stars
- Sequence of models calculated for different times in star’s life detail
evolutionary tracks in H-R diagram
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- Number of neutrinos created in hydrogen burning at center of Sun depends
on temperature
- About 1015 solar neutrinos flow through our bodies every
second.
- Neutrinos almost never interact with nuclei
- Right energy neutrinos can transform 37Cl17
nucleus to radioactive 37Ar18*
- Late 1960s experiment in 1-mile-deep South Dakota gold mine captured
solar neutrinos
- Capture signaled by radioactive decay of argon 37Ar18*
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- Experiment ran over two decades
- Measured about 1/3 number of solar neutrinos predicated from solar
model calculations
- Other experiments, but different methodology, started in late 1980s and
early 1990s confirm deficiency of solar neutrinos
- Two kinds of solutions proposed
- Theory of solar structure is inaccurate
- Neutrino particle theory needs revising (change types)
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- 1947 sunspot group
- 1.5 solar rotations
- White-light images, Mt. Wilson
Observatory
- Spectroscopy
- East limb, photospheric spectrum is blue-shifted
- West limb, photospheric spectrum is red-shifted
- Equatorial rotation velocity = 2 km/s
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- Equatorial period of rotation = 25 days
- Polar latitude period of rotation = 36 days
- Computer generated image of depth and latitude variations
- Red - faster rotation
- Blue - slower rotation
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- Photosphere = “light sphere” - layer responsible for solar luminosity
- Limb darkening - brightness of Sun fades from center toward limb
- Geometrical path lengthens from center toward limb
- Radiation comes from higher layers in photosphere toward limb
- Stefan-Boltzmann -temperature declines outward through photosphere
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- Photospheric absorption spectrum - several tens of thousands of
absorption lines
- Strongest - H and K lines, due to singly ionized calcium (Ca II)
- Hydrogen (H) Balmer series fairly strong
- Majority of lines due to neutral and singly ionized iron (Fe I and Fe
II)
- About 70 of 92 naturally occurring elements observed in photospheric
spectrum
- About 20 molecules are also observed
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- Analysis of the light coming from the Sun or stars is the only
diagnostic tool available for determining chemical composition.
- Spectroscopy of solar and stellar radiation followed by computer
analysis can yield chemical composition.
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- Stellar spectra are absorption spectra for which star’s photosphere is
intervening cool gas in Kirchhoff’s third law
- Stars and gaseous nebulae contain mixtures of chemical elements
- Each element emits or absorbs its own particular set of wavelengths
- Emission spectrum of known gas (neon or vaporized iron) provides
comparison lines of known wavelength against which wavelengths of unknown
solar or stellar lines can be determined
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- Measured wavelengths identify chemical elements present in the Sun or a
star
- Presence of absorption lines of particular element in sun’s
photospheric spectrum clearly indicate element is present
- Absence of absorption lines of particular element in sun’s photospheric
spectrum does not say element is not present
- Physical environment, temperature and density, determines whether or
not an element will absorbed radiation
- Chemical composition can be determined from spectrum and knowledge of temperature
and density of photosphere
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- Element Atomic Number % by Number % by Mass
- Hydrogen 1
90.9
70.7
- Helium 2
8.9
27.4
- Carbon 6
0.033
0.31
- Nitrogen 7
0.010
0.11
- Oxygen 8
0.077
0.95
- Neon 10
0.011
0.17
- Magnesium 12
0.003
0.06
- Silicon 14
0.003
0.07
- Sulfur 16
0.001
0.04
- Iron 26
0.003
0.14
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- Photospheric granulation - “rice-grained” pattern of convection cells
- Possess magnetic fields of several gauss averaged over large areas
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- Sunspots - cooler structures than normal photosphere
- Defined by magnetic field
- Properties of sunspots
- Observed in white light
- Average life about 6 days
- Size up to 10,000s km
- Dark umbra surrounded by striated penumbra
- Temperature about 1800o K cooler
- Magnetic fields up to several thousand gauss
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- Average large sunspot, but not a typical sunspot
- Scale-size is about 10,000 km
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- Sunspot cycle - roughly 11 year cycle
- Successive maxima are unequal
- Interval between successive peaks is not constant, 7 to 15 years
- Polarity (north or south seeking) of magnetic field reverses each cycle
- 22-year magnetic cycle far more repeatable than 11-year frequency cycle
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- Thin pinkish fringe extending beyond photosphere
- Taken during an eclipse
- Visible image
- Inset shows structure of chromosphere
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- Chromospheric emission spectrum
- Emission lines with some matching wavelengths of photospheric
absorption lines
- Bright yellow line produced by helium (He)
- Chromospheric temperature up to 30,000 K at highest level
- Gas density is lower than photosphere
- From this, one concludes that temperature must rise rapidly up through
chromosphere
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- Corona - halo of pale white glowing gas extending several solar radii
(several million kilometers) out from photosphere
- Coronal emission spectrum
- 30 emission lines in visible spectrum
- Hundreds of emission lines in ultraviolet and X-ray regions
- Emission lines originate in highly excited ions of familiar elements
- Temperature must be millions of degrees K to produce high degree of ionization
- Densities must be quite low compared to photosphere to produce emission
spectrum from gas that is transparent to photospheric radiation
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- Question - if temperature rises from photosphere, through chromosphere,
into corona, how is energy deposited in corona, since it is transparent
to photospheric radiation?
- Answer - energy is deposited from two sources
- Mechanical (acoustic) waves rise from photosphere into corona and
dissipate their energy
- Magnetic fields extending from photosphere into corona transfer energy
which is dissipated in corona
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- Faculae – white light version of plage
- Plages - hotter denser regions than normal chromosphere
- Lifetimes of about 40 days
- Magnetic fields up to several hundred gauss
- Size about 50,000 km
- Sunspot group - cooler structures than normal photosphere, defined by
magnetic field
- Flares - brief brightening in plages
- Lifetimes of about 20 minutes
- Size about 30,000 km
- Enhances particle density in solar wind and solar cosmic rays
- Filaments – prominence seen against disk
- Prominences - chromospheric material extending upward into corona,
magnetic structures
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- Flares - brief burst of X-rays and particle
- Observed in monochromatic light
- Lifetimes of about 20 minutes
- Size about 30,000 km
- Enhances particle density in solar wind and solar cosmic rays
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- Prominences - Chromospheric material extending upward into corona
- Seen against photospheric or chromospheric disk known as filaments
- Properties
- Much cooler than surrounding corona
- Sizes, if quiescent, height 30,000 km, length 200,000 km, thickness
5000 km
- Exhibit motions associated with magnetic fields up to several hundred
gauss
- Lifetimes up to 90 days
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- Holes - lower temperature and much lower density regions
- Sizes up to hundreds of thousands of km
- Magnetic field lines open out to interplanetary space
- Source of solar wind particles
- Changeable in periods of days to weeks
- Active regions - relatively hot and dense regions consisting of magnetic
loop structures
- Sizes up to hundreds of thousands of km
- Magnetic field lines form large loop structures
- Occur over chromospheric plages
- Quiet regions - between coronal holes and coronal active regions
- Magnetic fields weak and roughly in loop structures
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- A. Shows relatively quiet corona
- Black disk blocks photospheric and chromospheric radiation
- B. 16 minutes later, huge
balloon-shaped volume of high-energy gas is ejected from corona
- C. Ejected material expands at
typical velocities of 400 km/s
- Ejection lasts several hours and contains trillions of tons of matter
- Often associated with solar flares, but not always
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- Space weather – study of variable emission of high-energy photons, particles,
and magnetic fields and their interaction with the geosphere
- Earth influences
- Van Allen radiation belts
- Spacecraft and crews
- High-altitude aircraft
- Electric power grid
- Communications, land and satellite
- Major source of natural variability in terrestrial climate
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- The Sun continues to shine, while it radiates away as its luminosity, by
generating energy through thermonuclear fusion of hydrogen into helium.
- Gravitational and thermal equilibrium determine the Sun’s internal
structure and its rate of energy generation.
- The Sun’s atmosphere displays its own version of weather and climate,
governed by solar magnetic fields.
Solar weather has important influences on the Earth.
- The Sun is important not only as our source of light and heat, but also
because it is the only star near enough for us to study in great
detail. In the coming chapters,
we will use what we’ve learned about the Sun to help us understand other
stars.
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