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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

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