SOLAR LIFETIME VIA FUSION ENERGY GENERATION
Converting 4 H nuclei into one 4^He nucleus turns about
0.007 (0.7%) of their masses into energy.
Typical energy per nuclear reaction is 1 MeV or 1.6 x 10^{-6} erg
So number of reactions needed/second = Solar luminosity/Energy per reaction
No / sec = 4 x 10^{33} erg/s / 1.6 x 10^{-6} erg = 2.5 x 10^{39}/s
Roughly, one proton is used up per reaction and therefore
Mass used/sec = m_p x No /sec = (1.67 x 10^{-24} g) x
(2.5 x 10^{39}/s) = 4 x 10^{15} g/s
Solar lifetime = Solar mass/(Mass used/sec) = (2 x 10^{33} g)/
(4 x 10^{15} g/s)
= 5 x 10^{17}s = 1.6 x 10{10} years.
All of these numbers are approximate, the correct value is
just under 1.0 x 10^{10} years.
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THE SOLAR ATMOSPHERE
PHOTOSPHERE: visible, IR and UV continuum radiation streams out from here.
Thickness about 400 km
4500 < T < 5800 K; usually say T_s = 5760 K
density between 10^{-5} and 10^{-8} g/cm^3
emerging spectrum is continuum (from dense lower layer)
with superposed absorption lines (from less dense, cooler outer layer)
CHROMOSPHERE: mostly UV emission line radiation
Irregular thickness, averaging 5000 km in SPICULES
4500 < T < 10,000 K (up to 50,000 K in transition zone)
density averages around 10^{-10} g/cm^3
only visible when photosphere is obscured
CORONA: mostly X-ray emission
Irregular thickness, typically out to 2-3 times Solar radius
Average T = 1 x 10^6 K
extremely low density
only visible when photosphere is obscured or via X-ray telescopes
heated via magnetic energy orginating in the convective zone
of the sun:
probably by both magnetohydrodynamic shocks and
magnetic reconnection.
WIND: small amount of matter boiled off CORONA
Typical speed, 500 km/s (roughly the Sun's escape velocity)
Mostly protons, Helium-4 nuclei (also called alpha particles) and electrons
Continually hitting earth's magnetosphere
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THE SUN'S ATMOSPHERE IS VERY ACTIVE
Most spectacular are FLARES (very big) and PROMINENCES (big).
These can extend to 100,000 km or more into the corona.
Typically large amounts of matter following magnetic field
lines.
The energy is released by changes in magnetic field configurations.
Big flares yield COSMIC RAYS, charged particles
moving close to the speed of light.
Mostly protons, then electrons, alpha particles (4^He nuclei) and other nuclei
These cosmic rays can penetrate to the earth's atmosphere, yielding
spectacular auroral displays, power grid failures and disrupt
communications.
CORONAL MASS EJECTIONS (CMEs) involve a great deal of energy too.
CMEs are temporary features where matter flows out along open magnetic field lines.
These are less explosive than flares, and were unknown until satellites trained
UV and X-ray telescopes on the sun.
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The more mundane activity is shown by SUNSPOTS.
Measuring them proved that the Sun rotates differentially
(faster
at equator), and
is therefore a fluid.
Mean sidereal Period for the Sun is about 26 days.
The synodic period is a bit longer.
Sunspot number fluctuates, reaching a maximum every 11 years.
At minima, spots are further from the equator, and get closer
during maxima.
Magnetic polarities of spots reverse every 11 years so that
the
FULL SOLAR CYCLE is 22 years long.
I.e., if the N hemisphere
leading spots now are N poles,
the N hemisphere trailing spots are
S polls, BUT the S hemisphere leading spots
now are S poles, and the S
hemisphere trailing spots now are
N polls,
BUT 11 years from now the polarities are opposite.
Sunspots are dark because they are cooler
(roughly 4000 K
instead of 5760 for the rest of the photsphere).
This means
their fluxes (proportional to T^4)
are roughly a quarter as large,
so they are dark only in comparison
to the surrounding bright surface.
Sunspots are cooler mostly because their strong magnetic fields
(typically 300 Gauss vs 1 Gauss in the rest of the photosphere)
inhibit convection and therefore heat (and radiation) flow.
The magnetic fields also add a pressure that compensates for the lower thermal pressure in them.
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MAGNETIC FIELDS are produced only if all of these are present:
Differential rotation
Fluid (liquid, gas, plasma)
with magnetic properties: ionzied H for Sun, metallic H
for Jupiter and Saturn, molten iron/nickel outer core for Earth.
We didn't get to this last point in today's lecture and will cover it at the beginning of the next one.