The Sun and Stellar Structure

The Sun and Its Structure

This set of notes by Nick Strobel covers: The Sun, interiors of stars, and nuclear fusion. Parts of these notes will be in outline form to aid in distinguishing various concepts. As a way to condense the text down I'll often use phrases instead of complete sentences. The vocabulary terms are italicized.

Contents

The Sun--An Average Star

Index

A. Size

Biggest thing in solar system! (1,392,000 km diameter = 109 Earth diameters = 9.7 Jupiter diameters). Most massive thing in solar system! (333,000 Earth masses = 1046 Jupiter masses).

B. Composition

Spectroscopy shows that Hydrogen makes up about 94% of the solar material, Helium makes up about 6% of the sun, and all the other elements make up 0.13% (with Oxygen, Carbon, and Nitrogen the three most abundant ``metals''-they make up 0.11%). In astronomy, any atom heavier than Helium is called a ``metal''. Traces of Neon, Sodium, Magnesium, Aluminum, Silicon, Phosphorus, Sulfur, Potassium, and Iron. These percentages are by relative number of atoms. If use percentage by mass: H-78.5%, He-19.7%, O-0.86%, C-0.4%, Fe-0.14%, rest-0.54%.

C. Parts of the Sun

Index

Sun's Structure

    Core

  1. Core--innermost 10% of the Sun's mass. Where energy is generated. 16 million degrees and densities = 160 g/cm^3 (compare with Iron = 7 g/cm^3).

    Radiative Zone

  2. Radiative zone--includes core. Energy is transported from the superhot interior to the colder outer layers by photons. Makes up about 85% sun's radius.

    Convective Zone

  3. Convective zone--outer 15% of sun's radius. At cooler temperatures, more ions are able to block photon radiation more effectively, so nature kicks in convection to help energy transport.

    Photosphere

    Index

  4. Photosphere--``surface'' of sun. Is dense enough gas that we can't see through it and it gives off continuous radiation. About 5800 Kelvin.

    a.
    Ways of measuring temperature:
    • Wavelength of the peak (in centimeters) in the continuous spectrum = 0.3/[Temperature in Kelvin].

    • Measure flux--amount of energy passing through 1 cm^2 every second--of sunlight hitting the Earth. Use relation: Earth's solar flux = Sun's surface flux / (Earth distance)^2. This uses Inverse Square Law of Light Brightness--the apparent brightness (flux) of an object decreases with the square of the distance. For continuous radiation the flux at the surface of the emitter (here it's the sun) = sigma*Temperature^4. So we measure a solar flux on Earth = sigma*T^4 / 1A.U.^2. We know sigma--it's a constant of nature, Earth's solar flux, and 1 A.U. so we can solve for the temperature. Upper parts are cooler and less dense so we see absorption lines.

    b.
    Features on photosphere:
    i.
    Sunspots--cooler regions on sun (1000-1500 K cooler) so don't emit as much light therefore they are darker. Last few days to few months so we can map rotation of sun (first done by Galileo). Find solar equator rotates every 25 days while 30 degrees latitude takes 26.5 days and 60 degrees takes 30 days. Regions of strong magnetic field. Number of sunspots varies over 11 year cycle. At start of cycle (when #sunspots is minimum) most sunspots about 35 degrees from solar equator. At solar maximum (#sunspots is maximum) most sunspots about 5 degrees from solar equator. In one 11 yr cycle the leading sunspot in a sunspot group will have N magnetic pole while trailing sunspot will have S magnetic pole. The next 11 yr cycle the poles will switch for a total 22 yr cycle.

    ii.
    Granulation--bright spots of convection 700-1000 km across forming honeycomb pattern. Hot rising gas in middle of granule and cooler falling gas on border (convection). One granule can last about 8 minutes.

    Chromosphere

    Index

  5. Chromosphere--pinkish outer layer 2000-3000 km thick. Since the temperature rises outward, we see emission lines (mostly H-alpha line at 6563 Angstroms which is red).

    Corona

  6. Corona--very high temperature: 1-2 million degrees Kelvin! But very low density so it has a low amount of heat. Pearly white color seen in eclipses.
    a.
    At high enough temps. the atoms collide with each other with enough energy to eject electrons (ionization). At very high temps., things like Iron can have 9-13 electron ejected. Nine times ionized Iron only produced at temps. = 1.3*10^6 K. Also see 13 times ionized Iron (created at termperatures of 2.3*10^6 K!). During strong solar activity (see below) we see 14 times ionized Calcium (created at temperatures of 3.6*10^6 K!).

    b.
    Most of corona trapped close to sun by magnetic field line loops. In X-rays, those regions appear bright. Some magnetic field lines do not loop back to sun-in X-rays see ``coronal holes''.

    c.
    Solar wind--high temps. which means fast moving ions escape sun's gravitational attraction and move outward at 100's km/sec. Positive and negative charges spiral around magnetic field lines. When charged particles get near a planet with a magnetic field (e.g., the Earth), some of them are deflected around the planet and some are deflected to the planet's magnetic poles. When the charged particles hit the planet's atmosphere, they make the gas particles in the atmosphere produce emission spectra--the aurora borealis in the north and aurora australis in the south. Red aurorae produced by Hydrogren emission and green aurorae produced by Oxygen emission. The effects of the solar wind on the Earth is described more fully in the Space Weather page at Rice University (Houston, TX).

    d.
    What creates the high temperatures in the corona and chromosphere? Possibilities: sound shock waves and magnetic loops.

D. Solar Activity

Index

Solar Activity--varies with 11 yr sunspot cycle. At solar maximum there are more sunspots, prominences, flares, and aurorae on the Earth.

    Prominences

  1. Prominences--bright clouds of corona gas forming over sunspots so there is a magnetic connection. Quiet ones about 40,000 km high, corona gas falling back to photosphere. Sometimes see them looking like loops (remember that magnetic field lines loop). Last few months to one year. ``Surge'' ones have material erupting from photosphere shooting material up to 300,000 km above photosphere. Move along magnetic field lines.

    Solar flares

  2. Solar flares--even more extreme than surge prominences. Last only few minutes-hours. Lots of ions ejected. Interfere with radio communication. Sometimes cause voltage pulses/surges in power and telephone lines.

The Sun's Power Source

Index

The Sun produces a lot of light every second and it has been doing that for billions of years. How does it or any other star produce so much energy for so long? This section will try to explain it to you.

The first basic question about the sun is what powers it? It puts out A LOT of energy every second. How much? That's a good question. The answer from our measurements is 4*10^33 ergs per sec. An erg is unit of energy about equal to one flea hop. Since most people don't have a grasp of flea hop energy, I'll put the sun's total energy output (ie., its luminosity) in more familiar units. It is equal to 8*10^19 five Megawatt power plants (nuclear or hydroelectric) on the Earth. Our largest power plants now can produce around 5,000 Megawatts of power. Another way to look at this is that the sun puts out every second the same amount of energy as 2.5*10^12 of those five Megawatt power plants would put out every year. That's over two trillion-numbers like that on the Earth only come up when talking about the national debt!

Index

I know that you are just dying to know what powers that huge output, so I won't keep you in suspense any longer. Let's first rule out other likely candidates. How about chemical reactions? The most efficient chemical reaction is combining two Hydrogens to one Oxygen to make a water molecule plus some energy. Such a reaction has a very small efficiency (something like 1/10000000 of one percent). The efficiency means the net amount of energy I get out from the reaction after I've expended energy getting the reaction to happen in the first place. To find out how long the sun would last we would need to find out how much energy the sun has stored in its account and know how fast it makes withdrawals on its account. The amount of time it would last would be the energy stored divided by the rate of withdrawal. Makes sense, yes? The water reaction would only power the sun for about 10,000 years.

We need a reaction with a higher efficiency. How about the ultimate in efficiency-a matter-antimatter reaction with 100% efficiency. Such a reaction could power the sun for 10^13 years. Unfortunately, there are problems with this because the number of heavy particles in the sun must stay the same and very soon the matter-antimatter reaction would violate that rule and nature would not go for it.

Index

How about gravitational settling? This is a fancy way of referring to the converting of the potential energy of the falling layers to kinetic energy. When you hold a rock above the ground it has stored energy (``potential energy''--it has the potential to do some work). The stored energy is released as you let it fall. The rock gets kinetic energy because it is moving. Kinetic energy can heat things up. This is what would happen to the layers of the sun if they were to fall inward toward the center of the sun. The gas would be compressed and, therefore, would heat up. In addition to the expected heating the gas would also radiate. This was the idea physicists strongly argued for until the beginning of this century. This gravitational energy (with an efficiency of 1/10000 of one percent) could power the sun for 3*10^7 years--a nice long time except for the nagging but ever louder criticism of the biologists who needed more time for evolution to occur and the geologists who preferred the idea of unlimited age for the Earth but would stomach something like a few billion years for the age of the Earth. A good article on the age-of-the-Earth debate is in Scientific American August 1989 pages 90-96. Eventually physicists had to change their minds about the age of the sun (and Earth) as radioactive dating (something physicists believe is correct) indicated a 4.6 billion year age for the solar system and, therefore, the sun. It was the fact that the sun could not last long enough being powered by gravitational contraction or settling that motivated the search for nuclear power sources.

Index

We are left with nuclear power as the only thing left to power the sun. There are two types possible: fusion and fission. Fission produces energy by breaking up massive particles like uranium into less massive particles like Helium and Lead. Fusion produces energy by fusing together light particles like Hydrogen into more massive particles like Helium. Atomic power plants and the Atom Bomb use fission to get the energy. Stars and Hydrogen bombs use fusion. To get positively charged particles to fuse together, the electrical repulsion must be overcome (remember that like charges repel and opposite charges attract-something that rarely happens in human interactions). Once the positively charged particles are close enough together (within several 10^-13 centimeters of each other), the strong nuclear force takes over and is much more powerful than the electric force. The nuclei stick together. To get those particles close enough together requires high temperatures and high densities-something that occurs naturally in the cores of stars.

Fusion takes light particles whose combined mass is more than the resulting fused massive particle. The mass that was given up to form the massive particle was converted to energy. Remember E=mc^2? That tells you how much energy (E) can be made from matter with mass m. Remember that c is the speed of light and it's squared (!) so a little bit of mass can make a lot of energy. An example for fusion is the fusion process in the cores of main-sequence stars that takes four Hydrogen nuclei (protons) each with mass of one proton and fuses them to form a Helium nucleus (two protons and two neutrons) that has the mass of 3.97 times the mass of one proton. An amount of mass equal to 0.03 times the mass of one proton was given up and converted to energy equal to 0.03*(mass one proton)*c^2. The efficiency of this reaction is about 4/5 of one percent. The sun could last for about 10 billion years on hydrogen fusion in its core. This is plenty long enough to satisfy the modern geologists.

Index

The next basic question is why does nature use the long complicated proton-proton chain (or the longer Carbon-Nitrogen-Oxygen chain) for fusion? Nature uses a three step chain process to fuse four protons to make one Helium nucleus for the proton-proton chain process. Wouldn't it be much simpler if four protons would collide simultaneously to make one Helium nucleus? Simpler, but not very likely is the answer. Getting four objects to collide simultaneously is very hard to do-the chances of this happening are very very small (as one from a family of 8 boys I can attest to the difficulty of getting just half of us together for a mini family reunion!). The chances of this type of collision are too small to power the sun, so nature has found a trickier scheme. The chances of two particles colliding and fusing is much higher, so nature slowly builds up the Helium nucleus.

Nuclear fusion is something of a holy grail for utility companies because it produces no nasty waste products and has the potential of getting more energy out of it than you put in-free energy! Unfortunately, the conditions to get fusion to happen are very extreme by our standards. We've been only able to tap the fusion process with the Hydrogen bomb, but that's a one shot deal. The Hydrogen bomb still needs an atomic bomb trigger to get the extreme temperatures needed for the fusion process. At least we can get the waste product of the sun's fusion process for free with solar power collectors. The sun can have a controlled fusion process and not blow up all at once because of the hydrostatic equilibrium ``thermostat''.

Index

Hydrostatic equilibrium is the balance between the thermal pressures from the heat source pushing outwards and gravity trying to make the star collapse to the very center. I'll discuss hydrostatic equilibrium in more depth (no pun intended) in the next section. The nuclear fusion rate is very sensitive to temperature. It increases as roughly T^4 for the proton-proton chain and even more sharply (T^15) for the Carbon-Nitrogen-Oxygen chain. So a slight increase in the temperature causes the fusion rate to increase by a large amount and a slight decrease in the temperature causes a large decrease in the fusion rate.

Now suppose the nuclear fusion rate speeds up for some reason. Then the following sequence of events would happen: 1) Thermal pressure would increase causing the star to expand; 2) Star would expand to new point where gravity would balance the thermal pressure; 3) but Expansion lowers temperature in core-nuclear fusion rate slows down; 4) Thermal pressure drops and star shrinks; 5) Temperature rises and nuclear fusion rate increases; 6) Stability between nuclear reaction rates and gravity. A similar type of scheme would occur if the nuclear fusion rate were to slow down for some reason. The fusion rate stays approximately constant for stars that are fusing hydrogen to make helium + energy in the core. Once the hydrogen fuel in the core has been used up, hydrostatic equilibrium can no longer stabilize the star. What happens next will have to wait until we talk about stellar evolution.

Index

Here's a summary of fusion in outline form along with some discussion of a particle produced from fusion-the neutrino.

A. Timescale

Need energy source that lasts long time. Nuclear Fusion-lighter nuclei fuse together to form heavier nucleus + energy. The sum of the light nuclei masses = heavy nucleus mass + energy/c^2 (remember E=mc^2). The ``c'' is the symbol for the speed of light.

B. Chain Process

Use chain process to fuse Hydrogen to Helium. Chain process much more probable than all at once process. Proton-Proton chain and Carbon-Nitrogen-Oxygen chain process.

C. Mass Sensitivity

Sensitive to mass. More massmakesmore reactions. Main sequence type stars-hydrogen fusion powered.

D. Neutrinos

Index

Neutrino--massless (nearly??) particle traveling at speed of light (close to??) produced in nuclear reactions. More reactionsmeansmore neutrinos. Hardly interact with matter (low probability of interaction). Pass directly from core to us. Billions pass through us every second. If we could catch neutrinos, we could find out what it's like in Sun's interior just 8 1/3 minutes ago. The photons of light produced in the core take about a million years to percolate out to the surface. Increase odds of easy detection of a few neutrinos by using a LARGE amount of material that reacts with neutrinos in a certain way (Chlorine changes to radioactive Argon, Gallium and water molecules give off flashes of light).

E. Solar Neutrino Problem

Solar Neutrino Problem--we get only 1/3 the expected number of neutrinos! Possible reasons:
  1. Fusion is not sun's power source (not supported by other observations).

  2. Experiments not calibrated correctly (unlikely that all the carefully tuned apparati tuned in the same wrong way).

  3. Nuclear reaction rate lower than what our calculations say (possible but many people have checked and re-checked the physics of the reaction rates).

  4. Neutrinos change into other types of neutrinos that don't interact with the detection material during flight from Sun to Earth (idea gaining more and more advocates). Requires neutrino to have some mass. If the neutrino has mass, then it cannot travel at the speed of light, but can get darn close. Also a neutrino with mass has important consequences for the evolution of the universe (more about that later).

Interior Structure of Stars

Index

This section is about how we find out what the interior of a star is like without physically taking one apart (a rather difficult thing to do).

A. Mathematical Models

Use mathematical models: set of equations describing how things work. Since interior is gaseous, the equations are simple (whew!). Three parameters:
  1. Temperature--average kinetic energy of gas particles.

  2. Pressure--force/area. Hot gas wants to expand causing pressure. Example: The gas inside a hot air balloon pushes out on the material of the balloon enclosing the gas.

  3. Mass Density--mass/volume. Gas can be compressed to smaller volumescreatinglarger densities.

B. Equation of State

Index

Use Equation of State--equation relating density, pressure, and temperature. Gas has simple one (pressure = constant * mass density * temperature / molecular weight). For Hydrogen, the molecular weight is very close to 1; for Helium, the molecular weight is very close to 4. For a gas made of different types of atoms, the molecular weight is the weighted mean of the different atomic types, taking into account their relative number proportions.

C. Hydrostatic Equilibrium

Star held together by gravity. Gravity tries to compress everything to center. What holds star up (prevents total collapse)? Thermal pressure! Thermal pressure tries to expand star layers to infinity. In any given layer of star there is a balance between thermal pressure (outward) and weight of material above pressing downward (inward)--Hydrostatic Equilibrium. Deeper layers have more gravity compression from overlying layers (density increases). Need more pressure to balance-raise temperature. Find temperature at core = 8-28 million deg. K and densities = 10-130 g/cm^3. As stars age, these numbers increase! We've already seen in the previous section that hydrostatic equilibrium provides a ``thermostatic control'' on the energy generation and keeps star stable.

D. Other Pieces

Index

Other pieces to the models:
  1. Continuity of Mass: total stellar mass = sum of shell layer masses AND mass is distributed smoothly throughout star. Conservation of Mass: the total amount of mass does not change with time.

  2. Continuity of Energy: Amount of energy flowing out top of shell = amount energy flowing in at bottom of shell layer AND star luminosity = sum of shell layer energies. Conservation of Energy: the total amount of energy does not change with time.

  3. Energy Transport: Energy moves from hot to cold via conduction, radiation, or convection. Nature will first try using radiation. If radiation cannot transport all of the energy over the distance from the center to the surface of the star, then nature will also use convection. For stars conduction is not an efficient process so it transports a very small amount of energy.

  4. Put B, C, D together to form mathematical computer model.

F. Opaque Interior

Takes LONG time for photon produced in core to reach surface. Opaque interior-photon ionizes atom (photon gone), nucleus + electron(s) recombine and photons re-emitted in random direction, photon ionizes another atom, etc. Photon goes about 1 cm between ionizations. On average, photon moves outward, taking about 1 million years to go from the core where it was created to the surface where it is finally released.

Index

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last updated 19 Sept 95


Nick Strobel -- Email: strobel@astro.washington.edu

(206) 543-1979
University of Washington
Astronomy
Box 351580
Seattle, WA 98195-1580