Contents
SUN,
Star
that, by the gravitational effects of its mass, dominates the planetary
system that includes the earth. By the radiation of its electromagnetic
energy, the sun furnishes directly or indirectly all of the energy
supporting life on earth, because all foods and fuels are derived ultimately from plants using the energy of sunlight.
Because of its proximity to the earth, and because it is such a typical star,
the sun is a unique resource for the study of stellar phenomena. No
other star can be studied in such detail. The star closest to the sun
is located 4.3 light-years (4 × 1013 km/2.5 × 1013
mi) away. To observe features on its surface of comparable size to
those that can be seen routinely on the sun would require a telescope
almost 30 km (about 18.6 mi) in diameter. Such a telescope, moreover,
would have to be put into space to avoid distortions caused by the
earth's atmosphere.
For most of the time that humans have been on the
earth, the sun has been regarded as a celestial object of special
significance. Many ancient cultures worshiped the sun, and many more
recognized its significance in the cycle of life. Aside from its
calendrical or positional importance in marking, for example,
solstices, equinoxes, and eclipses, the quantitative study of the sun
dates from the discovery of sunspots, and the study of its physical
properties was not initiated until much later.
In 1611 Galileo using the recently invented telescope,
discovered dark spots on the sun. (Chinese astronomers also reported
sunspots as early as 200 BC.) Galileo's discovery
marked the beginning of a new philosophical approach to studying the
sun. The sun was finally viewed as a dynamic, evolving body, and its
properties and variations were thus able to be understood
scientifically.
The next major breakthrough in the study of the sun
came in 1814 as the direct result of the use of the spectroscope by the
German physicist Joseph von Fraunhofer. A spectroscope breaks up light
into its component wavelengths, or colors. Although the spectrum of the
sun had been observed as early as 1666 by the English mathematician and
scientist Sir Isaac Newton, the accuracy and detail of Fraunhofer's
work laid the foundation for the first attempts at a detailed
theoretical explanation of the solar atmosphere.
Some of the radiation from the visible surface of the
sun (called the photosphere) is absorbed by slightly cooler gas just
above it. Only particular wavelengths of radiation are absorbed,
however, depending on the atomic species present in the solar
atmosphere. In 1859, the German physicist Gustav Kirchhoff first showed
that the lack of radiation at certain wavelengths in the Fraunhofer
spectrum of the sun was due to absorption of radiation by atoms of some
of the same elements present on the earth. Not only did this show that
the sun was composed of ordinary matter, but it also demonstrated the
possibility of deriving detailed information about celestial objects by
studying the light the objects emitted. This was the beginning of
astrophysics.
Progress in understanding the sun has continued to be
guided by scientists' ability to make new or improved observations.
Among the advances in observational instruments that have significantly
influenced solar physics are the spectroheliograph, which measures the
spectrum of individual solar features; the coronagraph, which permits
study of the solar corona without an eclipse; and the magnetograph,
invented by the American astronomer Horace W. Babcock (1912--2003) in
1948, which measures magnetic-field strength over the solar surface.
The development of rockets and satellites has enabled scientists to
observe radiation at wavelengths not transmitted through the earth's
atmosphere. Among the instruments developed for use in space are
coronagraphs as well as telescopes and spectrographs sensitive to
extreme ultraviolet radiation and to X rays. Space instruments have
revolutionized the study of the outer atmosphere of the sun.
The total amount of energy emitted by the sun in the
form of radiation is remarkably constant, varying by no more than a few
tenths of 1 percent over several days. This energy output is generated
deep within the sun. Like most stars, the sun is made up primarily of
hydrogen (specifically, 71 percent hydrogen, 27 percent helium, and 2
percent other, heavier elements). Near the center of the sun the
temperature is almost 16,000,000 K (about 29,000,000° F) and the
density 150 times that of water. Under these conditions the nuclei of
individual hydrogen atoms interact, undergoing nuclear fusion. In this
process two hydrogen nuclei combine to make one helium nucleus, and
energy is released in the form of gamma radiation. This energy is
equivalent to that which would be released from the explosion of 100
billion one-megaton hydrogen bombs per second. The nuclear "burning" of
hydrogen in the core of the sun extends out to about 25 percent of the
sun's radius.
| BRIEF SURVEY OF THE SUN |
| Distance from earth |
|
| Minimum |
147,100,000 km (91,400,000 mi) |
| Maximum |
152,100,000 km (94,500,000 mi) |
| Rotation period at equator (sidereal day) |
25.38 earth days |
| Mass (earth = 1) |
332,900 |
| Radius at equator |
695,500 km (432,200 mi) |
| Mean density (earth = 1) |
0.255 |
| Surface gravity (earth = 1) |
28 |
| Typical size of: |
|
| Granulation |
2000 km (about 1240 mi) |
| Supergranulation |
30,000 km (about 18,600 mi) |
| Sunspot |
8000 km (about 5000 mi) |
| Approximate temperature |
|
| At center |
16,000,000 K (about 29,000,000° F) |
| At surface |
5800 K (about 10,000° F) |
| In sunspot |
4500 K (about 7600° F) |
| In chromosphere |
30,000 K (about 53,500° F) |
| In corona |
1,000,000 K (about 1,800,000° F) |
| Energy output |
3.83 × 1033 ergs/sec |
| Age |
4.5 billion years |
| Spectral type |
G2 |
The energy thus produced is transported most of the way
to the solar surface by radiation. Nearer the surface, however, in the
convection zone, covering approximately the last third of the sun's
radius, energy is transported by the turbulent mixing of the gases. The
photosphere is the top surface of the convection zone. Evidence of the
turbulence of the convection zone can be seen by observing the
photosphere and the atmosphere directly above it.
Turbulent cells in the photosphere give it an
irregular, mottled appearance. This pattern, known as solar
granulation, is caused by turbulence in the upper levels of the
convection zone. Each granule is about 2000 km (about 1240 mi) across.
Although the pattern of granulation is always present, individual
granules remain for only about 10 minutes. A much larger convection
pattern is also present, caused by the turbulence that extends deep
into the convection zone. This supergranulation pattern contains cells
that last for about a day and average 30,000 km (about 18,600 mi)
across.
Sunspots.
The American
astronomer George E. Hale discovered in 1908 that sunspots contain
strong magnetic fields. A typical sunspot has a magnetic-field strength
of 2500 gauss. For comparison, the earth's magnetic field has a
strength of less than 1 gauss. Sunspots tend to occur in pairs, with
the two spots having magnetic fields that point in opposite directions,
one into and one out of the sun. The sunspot cycle, in which the number
of sunspots varies from low to high and then low again over a period of
approximately 11 years, has been known since at least the early 18th
century. The intricate magnetic pattern associated with the solar
cycle, however, was found only after the discovery of the sun's
magnetic field.
Of sunspot pairs in
the sun's northern hemisphere, the spot that leads its partner in the
direction of rotation has a magnetic-field direction opposite to that
of a leading sunspot in the southern hemisphere. As a new 11-year cycle
begins, the magnetic-field direction of leading sunspots in each
hemisphere reverses. Thus, the full solar cycle, including the
magnetic-field polarity, takes approximately 22 years. In addition, the
sunspots on the sun at any given time tend to occur at the same
latitude in each hemisphere. This latitude moves from about 45° to
about 5° during the sunspot cycle.
Because each sunspot
exists for, at most, only a few months, the 22-year solar cycle
reflects deep-seated and long-lasting processes in the sun and not just
the properties of individual sunspots. Although not fully understood,
the phenomena of the solar cycle appear to result from the interactions
of the sun's magnetic field with the convection zone in the outer
layers of the sun. These interactions, furthermore, are affected by the
rotation of the sun, which is not the same at all latitudes. The sun
rotates once every 25.38 days near the equator, but a full rotation
takes up to 36 days near the poles.
Much of the sun's
magnetic field lies outside of sunspots. The pervasiveness of the sun's
magnetic field adds complexity, diversity, and beauty to the outer
atmosphere of the sun. For example, the larger-scale turbulence in the
convection zone pushes much of the magnetic field at and just above the
photosphere to the edges of the supergranulation cells. Radiation from
the layer just above the photosphere, called the chromosphere, clearly
shows the pattern. Within the supergranule boundaries, jets of material
shoot into the chromosphere to an altitude of 4000 km (about 2500 mi)
in 10 minutes. These so-called spicules are caused by the combination
of turbulence and magnetic fields at the edges of the supergranule
cells.
Near the sunspots,
however, the chromospheric radiation is more uniform. These sites are
called active regions, and the surrounding areas, which have smoothly
distributed chromospheric emission, are called plages, after the French
word for "beach." Active regions are the location of solar flares,
explosions caused by the very rapid release of energy stored in the
magnetic field (although the exact mechanism is not known). Among the
phenomena that accompany flares are rearrangements of the magnetic
field, intense X-radiation, radio waves, and the ejection of very
energetic particles that sometimes reach the earth, disrupting radio
communications and causing auroral displays.
The outer solar
atmosphere, which extends for several solar radii from the disk of the
sun, is the corona. All the structural details in the corona are due to
the magnetic field. Most of the corona consists of great arches of hot
gas: smaller arches within active regions and larger arches between
active regions. The arched and sometimes looplike shapes are caused by
the magnetic field.
In the 1940s the
corona was discovered to be much hotter than the photosphere. The
photosphere, or visible surface, of the sun has a temperature of almost
6000 K (10,300° F). The chromosphere, which extends for several
thousand kilometers above the photosphere, has a temperature near
30,000 K (near 53,500° F). But the corona, which extends from just
above the chromosphere far out into interplanetary space, has a
temperature of over 1,000,000 K (1,800,000° F). In order to maintain
this temperature, a direct input of energy to the corona is necessary.
Finding the mechanism
by which this energy reaches the corona is one of the classic problems
of astrophysics. It is still unsolved, although many mechanisms have
been proposed. Because recent observations from space have shown the
corona to be a collection of magnetic loops, how these loops are heated
has become a major focus of astrophysical research.
The magnetic field can
also trap cooler material above the sun's surface, although the cooler
material cannot remain stable there for more than a few days. These
phenomena can be seen during an eclipse as small regions, which are
called prominences, at the very edge of the sun, like jewels in a
crown. Frequently they subside, but occasionally they erupt, blowing
solar material into space.
Within one or two
solar radii from the surface of the sun, the coronal magnetic field is
strong enough to trap the hot, gaseous coronal material in large loops.
Farther away from the sun the magnetic field is weaker, and the coronal
gas can literally push the magnetic field out into space. When this
happens, material flows along the magnetic field for great distances in
the solar system. The constant flow of material pushing out from the
corona is called the solar wind, and it tends to come from regions
called coronal holes. The gas there is cooler and less dense than the
rest of the corona, resulting in less radiation. The solar wind from
large coronal holes (which can last for several months) is unusually
strong. Because of the solar rotation, these regions of strong solar
wind, called high-speed solar wind streams, tend to recur every 27 days
as seen from the earth. The solar wind causes disturbances that can be
detected in the earth's magnetic field.
The sun's past and
future have been inferred from theoretical models of stellar structure.
During its first 50 million years, the sun contracted to approximately
its present size. Gravitational energy released by the collapsing gas
heated the interior, and when the core was hot enough, the contraction
ceased and the nuclear burning of hydrogen into helium began in the
core. The sun has been in this stage of its life for about 4.5 billion
years.
Enough hydrogen is
left in the sun's core to last for at least another 4.5 billion years.
When that fuel is exhausted the sun will change: As the outer layers
expand to the orbit of the earth or beyond, the sun will become a red
giant star, slightly cooler at the surface than at present and 10,000
times brighter. It will remain a red giant, with helium-burning nuclear
reactions in the core, for only about half a billion years. The sun is
not massive enough to go through successive cycles of nuclear burning
or a cataclysmic explosion, as some stars do. After the red giant stage
it will shrink to a white dwarf star, about the size of the earth, and
slowly cool for several billion years.