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Searching for Solar Shocks

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The proper conservatism of L. Kelvin of Largs. Latent discoveries. X-rays (Roentgen, 1895) The ionosphere (Heaviside, 1902) Collisionless shock waves ... – PowerPoint PPT presentation

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Title: Searching for Solar Shocks


1
Searching for Solar Shocks
  • Including a brief history of
  • X-ray astronomy
  • H. Hudson, SPRC/UCSD/ISAS

2
Beautiful Chandra shock
(E0102-72)
3
How X-ray astronomy began
  • September 21, 1859 (Carrington)
  • Kew Gardens - magnetic effects
  • The proper conservatism of L. Kelvin of Largs

4
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5
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6
Latent discoveries
  • X-rays (Roentgen, 1895)
  • The ionosphere (Heaviside, 1902)
  • Collisionless shock waves - ?
  • Space weather - ??

7
Oliver Heaviside
  • Maxwells equations
  • Laplace transforms
  • The Heaviside function
  • Telegraph equation - Pupin Laboratory
  • Heavy opposition to quaternions
  • T.S. Eliot, Cats, Journey to the Heaviside
    Layer
  • Not the father of X-ray astronomy (due credit to
    B. Rossi, of course)
  • Why should I refuse a good dinner simply because
    I don't understand the digestive processes
    involved.

8
Were in a golden era of coronal observation
9
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10
The dynamic corona
11
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12
The boundary between Photosphere and corona
  • Density plummets precipitously
  • Collisionality diminishes
  • Radiation decouples
  • Plasma beta drops drastically

13
T.R.
T
B
0
Height in corona
14
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15
Solar shock Type II burst
16
A Type II burst is the same thing as a slow
drift burst - perhaps discovered by early
military radars explained by J. P. Wild and Y.
Uchida
(recall l-2 ne)
III
Wavelength
II
Time
17
Meter-waves and soft X-rays
  • Megahertz vs Exahertz
  • Radiative transfer vs direct view
  • Magnetic effects vs Bremsstrahlung
  • Inherent fuzziness vs sharp resolution
  • But - by 1998, wed seen Types I, III, IV and
    others

18
But not the simplest and most obvious Type II!
19
X-ray observation of a global wave
  • Wave propagation tells us about coronal structure
  • The innermost (earliest) motions tell us about
    the flare process itself

20
Moreton-Ramsey wave and EIT wave
21
Why didnt SXT discover SXT waves?
  • SXT views the whole corona
  • Fast-mode MHD waves must involve compressional
    heating
  • SXT response increases monotonically with
    temperature
  • So why did it take 8 years and the competitive
    example of EIT?

22
Factors abetting wave detectionin soft X-rays
  • The wave neednt be shocked
  • The SXT response strongly favors detection of a
    temperature increase (adiabatic law)

23
Sensitivity estimation
2
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24
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25
SXT and TRACE responses
Courtesy N. V. Nitta
26
Factors reducing sensitivity
  • Poor CCD dynamic range (AEC)
  • Limited SXT telemetry(Velocity filter)
  • Photon counting statistics
  • Scattering from grazing-incidence mirror
  • Flare mode

27
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28
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29
May 6, 1998
FOV 10 arc min
30
FOV 5 arc min
31
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32
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33
Gas pressure in flare loops
34
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35
SOHO/ EIT
36
Uchidas 1968 model
37
A.R.
Uchida
S.W.
38
OK, so what caused the wave?
  • In principle we can see it all in soft X-rays
  • The earliest manifestation of the wave is within
    20,000 km of the flare core
  • But it is significantly displaced from the soft
    X-ray core of the flare

39
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40
Mysteries of low b plasma
  • Everything seems to expand (cf. Aly)
  • The Virial Theorem looks goofy too

41
Implosion conjecture
  • At low b, the coronal energy is purely B2/8p
  • During a flare, theres no time for energy
    transport through the photosphere
  • Therefore, some field lines must shorten

42
Open field lines
Closed field lines
Isomagnetobars
How low-b implosions must work
43
MHD Virial Theorem
44
The end, thanks
45
The end, thanks
46
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