Main+Sequence+Stars+1B

The Main Sequence
The properties of a main sequence star can be understood by considering the various physical processes acting in the interior. First is the hydrostatic balance, also called hydrostatic equilibrium. This determines the [|density] structure of the star as the internal pressure gradient balances against the force of gravity. Another way of thinking about this is to imagine the star as a large number of nested thin spherical shells (sort of like an onion). The inward forces on each shell consist of the gravitational pull from all the shells inside it, and the gas and radiation pressure on the outside of the shell. The only outward force on each shell is the gas and radiation pressure on the inside of the shell; there is no gravitational force from material outside the shell (this is known as Gauss's theorem). In hydrostatic equilibrium, the inward and outward forces must balance. If they don't, the shell will either collapse or expand. The timescale for this to occur is called the 'free-fall timescale', and it is about 2000 [|seconds] for a star like the Sun. Since we know the Sun has been more or less stable over the age of the Earth (several billion years), the hydrostatic balance must be maintained to a very high accuracy. A consequence of hydrostatic balance is that the pressure on each shell from material outside it must be less than the pressure from material inside it. This is because gravity acts only in the inward direction. Thus, the pressure in the star must decrease with increasing radius. This is an intuitively obvious result; the pressure at the center of the star is greater than it is at the surface. [|Diagram of a Solar-type Star] || The second physical process to consider is the transport of energy from the interior of the star to the edge. The interior of the star (that is, near the center) is heated by nuclear reactions, while at the surface of the star electromagnetic radiation can escape essentially freely into space. This situation is analogous to a pot of water on a stove, in which heat is deposited at the bottom by the stove burner, and is transported upward through the water to the surface where it can escape. The rate at which the water on the stove can transport the heat determines the temperature; a lid on the pot will cause the temperature in the water to be higher than it would be with no lid, since heat is impeded from escaping the pot. In the case of a star, the temperature of the gas determines the density structure via the hydrostatic equilibrium condition, so understanding the transport is important. The transport can occur by either of two mechanisms: either the energy is carried by radiation, or it is carried by convection. Radiation is the mechanism by which the Earth receives heat from the Sun, and its efficiency depends on the [|opacity] of the material that the radiation must traverse. Opacity is a measure of the transparency of a gas, and it depends on the gas temperature, density, and [|elemental] composition in a complicated way. Convection is analogous to the turbulent motion in a pot of water as it boils. It involves motion of the fluid in the pot (or the interior of the star) which transports heat. The operation of convection depends on how easily the gas can move, i.e. its viscosity and any forces (such as gravity) which tend to resist the convective motion. In addition, convection can only operate if it transports more heat than radiation. This turns out to be important! When the opacity is high (and radiation is inefficient), convection takes over. The details of the efficiency of convection are not well understood, and they are probably the major source of uncertainty in the study of stellar structure and evolution. A third energy transport mechanism, conduction, is relatively unimportant in stellar interiors. Main sequence stars have zones (in radius) which are convective, and zones which are radiative, and the location of these zones depends on the behavior of the opacity, in addition to the other properties of the star. Massive stars (i.e., greater than several solar [|masses]) are convective deep in their cores, and are radiative in their outer layers. Low mass stars (i.e., mass comparable to the Sun and below) are convective in their outer layers and radiative in their cores. Intermediate mass stars (spectral type A) may be radiative throughout. Convection is likely to be important in determining other properties of the star. The existence of a hot [|corona] may be associated with active convection in the outer layers, and the depth of the convective layer determines the extent to which material from the deep interior of the star is mixed into the outer layers. Since interior material is likely to have undergone nuclear reactions, which change the elemental abundances, this mixing affects the abundances in the star's [|atmosphere]. These can be observed by studying stellar spectra. They may also be ejected from the star in a [|stellar wind], and so affect the composition of interstellar gas. The final ingredient in determining the structure of a main sequence star is the source of heat in the interior, nuclear reactions. There are many of these, and the details are complicated and there is still some uncertainty about the exact rates for the reactions (for example, the solar [|neutrino] problem). The basic reactions which operate on the main sequence are [|fusion] reactions which convert [|hydrogen] nuclei (protons) into [|helium] nuclei. These reactions require very high temperatures (greater than 10 million degrees) and densities (greater than 10,000 gm per cubic centimeter), and the rates are very sensitive functions of temperature and density. This is the factor which ultimately determines the lifetime of a main sequence star. More massive stars have greater central temperatures and densities and so exhaust their nuclear fuel more rapidly (in spite of the fact that they have more of it) than do lower mass stars. It turns out that the main sequence lifetime is a sensitive function of mass. For a star like the Sun the main-sequence stage lasts about 10,000,000,000 years, whereas a star 10 times as massive will be 1,000 to 10,000 times as bright but will only last about 20,000,000 years. A star one tenth of the Sun's mass may only be 1/1,000th to 1/10,000th of its brightness, but will last about 1,000,000,000,000 years. It is interesting to consider what would happen to the star if the nuclear reactions were to suddenly turn off. The timescale required for the energy from a [|photon] released at the center of the star to make its way to the surface is approximately 1,000,000 years for the Sun. Along the way, the original gamma-ray photon interacts with the gas in the Sun and loses energy. Through multiple interactions like this, this energy "random walks" its way out of the Sun, ultimately being emitted at the surface as many UV and optical photons. Thus, if the nuclear reactions were to turn off today, the Sun's [|luminosity] would stay approximately constant for a long time by human standards. We do have historical records which tell us that the Sun's output has been approximately constant over the course of written human history, so we feel fairly confident that the nuclear reactions are still operating. However, there is the possibility that nuclear energy generation in the center of the Sun is not perfectly constant in time. The three physical processes discussed so far, hydrostatic equilibrium, radiation transport, and nuclear energy generation, serve to determine the structure of a star. As with most things, the devil is in the details, and the areas of greatest uncertainty are the behavior of opacity and convection. These are active areas of scientific research. A convenient way to characterize a star from observations is by its luminosity and its color (or temperature). It is customary to plot these two quantities in an x-y plot, called a Hertzsprung-Russell diagram (after its inventors). It turns out that when this is done for main sequence stars with a range of masses, the points tend to occupy a narrow band in the diagram. The location of a main sequence star in the diagram depends only on its mass (see Figure below). The Hertzsprung-Russell Diagram
 * [[image:http://imagine.gsfc.nasa.gov/Images/science/sun_parts_small.gif caption="Sun Parts" link="http://imagine.gsfc.nasa.gov/docs/science/know_l2/sun_parts.html"]]