Lecture 5

The Internal and Surface Structure of the Sun

(Click here for diagram.)

I. Internal Structure of the Sun

A.  Core:  inner ~1/5 solar radius where the Sun's energy production takes place; core temperature = 15 million K, core density = 100 x density of water, core pressure = 200 billion x surface pressure of Earth; composition mostly hydrogen in gaseous (ionized gas = plasma) form
1.  energy source:  nuclear fusion (light nuclei combine to form heaver nuclei); the overall reaction for the Sun results in 4 hydrogen nuclei combining to form 1 helium nucleus + energy; each helium nucleus produced is slightly less massive than the combined mass of the 4 hydrogen nuclei (~0.7% less), this so called "mass deficit" is coverted into energy as described in Einstein's equation:  E = mc2
2.  proton-proton chain = specific nuclear reaction which provides the majority of the Sun's energy:
step 1:   1H + 1H ->2H + e+ + neutrino  (e+ +  e- -> gamma ray photon)
step 2:   1H + 2H ->3He + gamma ray photon
step 3:   3He + 3He ->4He + 1H + 1H
Note 1:  steps 1 & 2 happen twice for each step 3 reaction; bottom line, 41H combine to form 14He with the release of energy
Note 2:  IMPORTANT: The fusion reactions in the Sun and other stars would not be sustainable if not for a quantum mechanical process known as "quantum tunneling".  At the energies found in the cores of stars, the protons and other nuclei involved in the fusion reactions could not get past their mutual replusion (due to their positive charges = "Coulomb barrier") in sufficient numbers to sustain the nuclear reactions without this quantum effect.
3.  600 million tons of hydrogen are converted into 596 million tons of helium every second in the core of the Sun, the "missing" 4 million tons of mass is converted into energy ( E = mc2 ) = 3.8 x 1026 joules every second; in other words, the Sun has a radiant power output (luminosity) of  3.8 x 1026 watts
4.  the rate of energy production in the core depends on the temperature and density in the core; the Sun is in hydrostatic equilibrium which means that the pressure generated by the energy production in the core is just balanced by the weight of the overlying layers; this "contest" between pressure and weight (gravity) acts like a "thermostat" and controls the rate of energy production and the overall structure of the Sun (this is true for all stars as well) - for example:  if the fusion rate decreased slightly -> pressure would decrease -> gravity would cause the Sun to contract slightly -> density and temperature would increase in the core -> the fusion rate would increase -> pressure would increase and the Sun would stop contracting
B.  Radiative zone:  from the center of the Sun out to a position about 1/3 the solar radius below the surface, conditions in the  plasma are stable against convection and the energy created in the core is transported outward by photons (ie:  by radiation)
1.  gamma ray photons created by the nuclear reactions in the core are scattered or absorbed and reemitted by the particles in the plasma as they make their way through the radiative zone; one gamma ray photon becomes many lower energy photons by the time they reach the photosphere (total energy of the lower energy photons sum to the energy of the original gamma ray photon)
2.  the total time it takes for the photon created in the core to complete the "random walk" process out to the surface (described in 1. above) is on the order of one million years; this "random walk" process is know as radiative diffusion
C.  Convective zone:  in the outer ~1/3 of the solar radius, the conditions in the plasma allow for the process of convection to transport the energy to the surface
1. convection occurs when conditions in a fluid material are such that a parcel of the material can't lose its heat energy to the surrounding material very quickly by conduction or radiation, then the parcel becomes hotter than the surrounding material, becomes less dense and begins to rise like a hot air balloon, carrying its heat energy upwards by mass motions
2.  when the material reaches the surface it radiates away some of its heat energy and cools, sinking down around the rising column of hot material, this is called a convection cell and we see the top of these cells in the photosphere as solar granulation
D.  Determining the interior structure of the Sun
1.  our knowledge of the interior structure of the Sun (for that matter, all stars) is determined mainly by computer models which use the laws of physics and the measurable global and surface properties to calculate the temperature, density, pressure, energy production and even changes in composition due to nucleosynthesis (fusion reactions) as a function of the radius
2.  the measurable properties of the Sun which we measure to calculate the interior model include:  total solar mass, average mass density, radius, total luminosity, surface temperature, surface pressure, surface density
3.  there is one direct measurement of conditions in the core of the Sun:  the neutrino flux from the fusion reactions that occur in the core; neutrinos are subatomic particles that only weakly interact with normal matter, a typical neutrino could fly through 6 trillion miles of lead without being absorbed; about 2% of all the energy produced by the solar nuclear reactions are carried off as neutrinos; there are three different types of neutrinos
a.  the solar neutrino problem:  for many years there have been devices (neutrino telescopes) that could detect the neutrino flux from the Sun; none of these neutrino telescopes have ever detected the number of neutrino from the Sun expected from the standard solar model
b.  recently researchers have determined that the neutrino is NOT a massless particle (like the photon), this implies that the neutrino can change type in flight and explains the deficit in the neutrino count measured at neutrino telescopes; the solar neutrino problem was caused by our incomplete understanding of the physics of neutrinos rather than the physics of the standard solar model

II.  The Surface Structure of the Sun:  the Photosphere

A.  Photosphere:  the visible surface of the Sun, actually the top ~400 km of the convective zone where most of the photons escape out into space; photosphere average temperature = 5800 K, composition of Sun (as measured in the photosphere) = 70% hydrogen, 28% helium, 2% heaver elements by mass, radius of Sun (to photosphere) = 696,000 km
1.  limb darkening:  as we observe the Sun in visible light (using the necessary filters!) the surface brightness falls off from the center towards the edge (limb); the light we see coming from the center of the disk is escaping from a deeper (hotter) level in the photosphere than the light we see from the limb; from the Stefan-Boltzmann law we know that the power emitted per unit area is a strong function of the absolute temperature, therefor we see brighter (more power per unit area) light from the deeper (hotter) levels that we sample near the center of the disk than the higher (cooler) levels that we sample near the limb
2.  granulation:  the photosphere is the top layer of the convective zone and the surface expression of the convection cells are roughly hexigonal bright patches with darker edges; the brighter center of the patch is due to the hot upwelling column of gas and the darker rim is the cooler sinking material; as seen from the Earth through a telescope, these ever-changing patches give the Sun's surface a grainy appearance, hence the term granulation
B.  Sunspots, the 11 year sunspot or solar activity cycle and the 22 year solar magnetic cycle
1.  sunspots:  cooler (4000 K) regions of intense magnetic field strength in the photosphere that look dark compared to the surrounding 6000 K photosphere; sometimes referred to as "magnetic storms" due to the high field strength and accompanying solar activity
2.  the number of sunspots observed in the photosphere and occurances of energtic solar activity associated with them wax and wane with a period of approximately 11 years; at a sunspot minium there are few sunspots, they begin to form at high solar latitudes and as the cycle progresses, larger numbers are observered at the mid-latitudes, then as the numbers decrease they are found closer to the equatorial region, as the cycle begins to repeat they are again observed at high latitudes
3.  sunspots activity is associated with the solar magnetic field; sunspots appear in groups of at least 2 and each sunspot has a magnetic polarity (ie:  either a "north magnetic pole" or a "south magnetic pole") with one polarity associated with the leading (toward the direction of solar rotation) sunspots of the group and the other with the trailing sunspots, whatever the polarity of the sunspot groups in the northern hemisphere, it is reversed in the southern hemisphere (if the polarity is [- +] to the north, then the polarity is [+ -] to the south; it is thought that the differential rotation of the Sun (~28 days near the equator, ~36 days near the pole) "winds" the Sun's magnetic field as its plasma drags the magnetic field lines with it (see lecture 6 for a discussion of magnetic field lines); eventually during an 11 year sunspot cycle the process causes the Sun's global magnetic field to reverse in polarity, the polarity reverses back again during the next 11 year cycle ending a 22 year solar magnetic cycle
C.  Solar seismology and the convection zone:  the churning motion of the convection zone drives oscillations of the fluid surface of the Sun; a standing wave pattern developes (like the vibrational pattern that occurs on a drumhead when hit by a drumstick), this standing wave pattern can be observed by measuring the up-and-down motions of the plasma in the photosphere with spectrographs (see doppler shifts) and there is a global network of telescopes for continuous time coverage of the pattern; analysis of this pattern allows astronomers to determine the internal rotation rate of the Sun and the distribution of sizes of convection cells and test other models about the convection zone