Chapter 15--Our Sun - Geological Sciences
Chapter 15--Our Sun - Geological Sciences
Chapter 15--Our Sun - Geological Sciences
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electron neutrinos. However, recent experiments have shown<br />
that some of the electron neutrinos might change into muon<br />
and tau neutrinos as they fly out through the solar plasma.<br />
In that case, our detectors would count fewer than the expected<br />
number of electron neutrinos. Early results from<br />
the Sudbury Neutrino Observatory in Canada, a new detector<br />
designed to search for all types of neutrinos, suggest<br />
that neutrinos changing type is indeed the solution to the<br />
solar neutrino problem. The observations are ongoing, and<br />
it will probably be several more years before this solution<br />
can be definitively confirmed.<br />
Because of their roles in detecting solar neutrinos and<br />
identifying the solar neutrino problem, Raymond Davis,<br />
leader of the Homestake experiment, and Masatoshi Koshiba,<br />
leader of Super-Kamiokande, shared in the 2002 Nobel<br />
Prize for physics.<br />
<strong>15</strong>.4 From Core to Corona<br />
Energy liberated by nuclear fusion in the <strong>Sun</strong>’s core must<br />
eventually reach the solar surface, where it can be radiated<br />
into space. The path that the energy takes to the surface<br />
is long and complex. In this section, we follow that<br />
long path.<br />
The Path Through the Solar Interior<br />
In <strong>Chapter</strong> 6, we discussed how atoms can absorb or emit<br />
photons. In fact, photons can also interact with any charged<br />
particle, and a photon that “collides” with an electron can<br />
be deflected into a completely new direction.<br />
Deep in the solar interior, the plasma is so dense that<br />
the gamma-ray photons resulting from fusion travel only<br />
a fraction of a millimeter before colliding with an electron.<br />
Because each collision sends the photon in a random new<br />
direction, the photon bounces around the core in a haphazard<br />
way, sometimes called a random walk.With each<br />
random bounce, the photon drifts farther and farther,<br />
on average, from its point of origin. As a result, photons<br />
from the solar core gradually work their way outward (Figure<br />
<strong>15</strong>.13). The technical term for this slow, outward migration<br />
of photons is radiative diffusion (to diffuse means<br />
to “spread out” and radiative refers to the photons of light<br />
or radiation).<br />
Along the way, the photons exchange energy with their<br />
surroundings. Because the surrounding temperature declines<br />
as the photons move outward through the <strong>Sun</strong>, they<br />
are gradually transformed from gamma rays to photons<br />
of lower energy. (Because energy must be conserved, each<br />
gamma-ray photon becomes many lower-energy photons.)<br />
By the time the energy of fusion reaches the surface, the<br />
photons are primarily visible light. On average, the energy<br />
released in a fusion reaction takes about a million years<br />
to reach the solar surface.<br />
Figure <strong>15</strong>.13 A photon in the solar interior bounces randomly<br />
among electrons, slowly working its way outward in a process<br />
called radiative diffusion.<br />
Radiative diffusion is just one type of diffusion. Another is the<br />
diffusion of dye through a glass of water. If you place a concentrated<br />
spot of dye at one point in the water, each individual dye<br />
molecule begins a random walk as it bounces among the water<br />
molecules. The result is that the dye gradually spreads through<br />
the entire glass. Can you think of any other examples of diffusion<br />
in the world around you?<br />
Radiative diffusion is the primary way by which energy<br />
moves outward through the radiation zone, which stretches<br />
from the core to about 70% of the <strong>Sun</strong>’s radius (see Figure<br />
<strong>15</strong>.4). Above this point, where the temperature has<br />
dropped to about 2 million K, the solar plasma absorbs photons<br />
more readily (rather than just bouncing them around).<br />
This point is the beginning of the solar convection zone,<br />
where the buildup of heat resulting from photon absorption<br />
causes bubbles of hot plasma to rise upward in the process<br />
known as convection [Section 10.2].Convection occurs<br />
because hot gas is less dense than cool gas. Like a hot-air<br />
balloon, a hot bubble of solar plasma rises upward through<br />
the cooler plasma above it. Meanwhile, cooler plasma from<br />
above slides around the rising bubble and sinks to lower<br />
layers, where it is heated. The rising of hot plasma and sinking<br />
of cool plasma form a cycle that transports energy outward<br />
from the top of the radiation zone to the solar surface<br />
(Figure <strong>15</strong>.14a).<br />
The Solar Surface<br />
THINK ABOUT IT<br />
Earth has a solid crust, so its surface is well defined. In<br />
contrast, the <strong>Sun</strong> is made entirely of gaseous plasma. Defining<br />
where the surface of the <strong>Sun</strong> begins is therefore something<br />
like defining the surface of a cloud: From a distance<br />
it looks quite distinct, but up close the surface is fuzzy, not<br />
sharp. We generally define the solar surface as the layer that<br />
appears distinct from a distance. This is the layer we identified<br />
as the photosphere when we took our imaginary journey<br />
into the <strong>Sun</strong>. More technically, the photosphere is the<br />
layer of the <strong>Sun</strong> from which photons finally escape into<br />
space after the million-year journey of solar energy outward<br />
from the core.<br />
508 part V • Stellar Alchemy