The Sun 73
10
-3
A
10
-2
A
10
-1
A
1 A 10 A 10
2 A
10
3 A
1
∝m
10
∝m
10
2
∝m
1 mm 1 cm 10 cm 1 m 10 m
10
21
Hz
10
20
Hz
10
19
Hz
10
18
Hz
10
17
Hz
10
16
Hz
10
15
Hz
10
14
Hz
10
13
Hz
10
3 GHz
10
2 GHz
10 GHz1 GHz100 MHz
10 -20
10 -19
10 -18
10 -17
10 -16
10 -15
10 -14
10 -13
10 -12
10 -11
10 -10
10 -9
10 -8
10 -7
10 -6
10 -5
10 -6
10 -5
10 -4
10 -3
10 -2
10 -1
1
10
100
103
104
105
106
107
SPECTRAL IRRADIANCE (erg cm
-2
s
-1
∝
m
-1
)
WAVELENGTH
FREQUENCY
GAMMA RAY X RAY
ULTRA
VIOLET
VISIBLE
INFRARED
RADIO
LARGE BURST
(3B FLARE, 8/4/72)
(NONTHERMAL)
NON-FLARE
CONDITIONS
1B FLARE
POSTFLARE
2B FLARE
QUIET SUN
QUIET SUN
(THERMAL)
LARGE STORM
(NONTHERMAL)
SLOWLY-VARYING
S-COMPONENT
ACTIVE REGIONS
(THERMAL)
GRADUAL
BURST
(NONTHERMAL)
LARGE BURST
3B FLARE, 8/1/72
(NONTHERMAL)
LARGEST BURST
REPORTED
(NONTHERMAL)
FIGURE 2 The solar irradiance spectrum from gamma rays to radio waves. The spectrum is
shifted by 12 orders of magnitude in the vertical axis atλ=1 mm to accommodate for the large
dynamic range in spectral irradiance. (Courtesy of H. Malitson and NASA/NSSDC.)
by ionized plasma in the coronal temperature range of
∼1–2 million K. Emissions in shorter wavelengths require
higher plasma temperatures and thus occur duringflares
only. Flares also accelerate particles to nonthermal ener-
gies, which cause emission in hard X-rays, gamma rays, and
radio wavelengths, but to a highly variable degree.
2. The Solar Interior
The physical structure of the solar interior is mostly based
on theoretical models that are constrained (1) by global
quantities (age, radius, luminosity, total energy output; see
Table 1); (2) by the measurement of global oscillations