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Space physics EF2245 Tomas Karlsson Space and Plasma Physics School of Electrical Engineering. EF2245 Space Physics 2010. Course goals After the course the student should be able to describe and explain basic processes in space plasma physics - PowerPoint PPT Presentation
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Space physicsEF2245
Tomas Karlsson
Space and PlasmaPhysics
School of Electrical Engineering
EF2245 Space Physics 2010
Activity Date Time Room Subject (preliminary) Litterature
L1 25/10 10-12 Sem. Introduction, Solar wind KR Ch. 1-2, 4 L2 1/11 10-12 Sem. Solar wind, cont., Shocks KR Ch. 4, 5 T1 4/11 10-12 Sem. L3 8/11 10-12 Sem. Solar wind interaction with
celestial bodies KR Ch. 6, 8, 15 (p 503-510)
Distribution of Assignment 1
8/11
T2 11/11 10-12 Conf. L4 15/11 10-12 Sem. Ionospheres KR Ch. 7 T3 18/11 10-12 Sem. Deadline, Assignment 1
18/11 10.00
L5 19/11 10-12 Sem. Ionospheric electrodynamics
RB.
L6 22/11 10-12 Sem. The magnetopause and magnetotail
KR Ch. 9
Distribution of Assignment 2
22/11
T4 25/11 10-12 Sem. L7 26/11 10-12 Sem. The magnetosphere and its
dynamics KR Ch. 10, 13
L8 29/11 10-12 Sem. Alfvén waves, ULF pulsations and global oscillations of the magnetosphere
KR Ch. 11, 14
Deadline, Assignment 2
29/11 10.00
T5 2/12 10-12 Sem. L9 3/12 10-12 Sem. Auroral physics KR Ch. 14, LL L10 6/12 10-12 Sem. Auroral physics, cont. KR Ch. 14, LL T6 9/12
10-12 Sem.
Examination 13/12 14-19 Sem.
Space physics EF2245
EF2245 Space Physics 2010
Course goals
After the course the student should be able to
• describe and explain basic processes in space plasma physics
• use established theories to estimate quantitatively the behaviour of some of these processes
• make simple analyses of various types of space physics data to compare with the quantitative theoretical predictions
• describe some hot topics of today’s space physics research
Litterature
Kivelson, M.G., and C. T. Russel (ed.), Introduction to Space Physics, Cambridge Univeristy Press.
Boström, R., Electrodynamics of the Ionosphere, in Cosmical Geophysics, Ed. Egeland et al.
Lyons, L., Formation of Auroral Arcs via Magnetosphere-Ionosphere Coupling, Reviews of Geophysics, 30, 2, 93-112, 1992.
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L
x
d
EF2245 Space Physics 2010
Plasma frequency
Single particle motion
EF2245 Space Physics 2010
,0,x zE EE
Consider a charged particle in a magnetic field.
y
xB = Bz z
+
Assume an electric field in the x-z plane:
dm q
dt
vv B E
xy x
yx
zz
dvm qv B qE
dtdv
m qv Bdt
dvm qE
dt
Constant acceleration along z
22
2
2 22
2 2
y yxg g x
y x xg g y x
dv dvd v qBv
dt m dt dt
d v dv dvqB q Bv E
dt m dt dt m
Drift motion
EF2245 Space Physics 2010
22
2
2 22
2 2
y yxg g x
y x xg g y x
dv dvd v qBv
dt m dt dt
d v dv dvqB q Bv E
dt m dt dt m
22
2
2
22
xg x
xy
xg y
d vv
dtE
d vEB
vdt B
g x
g y
i t
x
i txy
v v e
Ev v e
B
Average over a gyro period:
, 2 2
yx x zdrift y
E E Bv
B B B
E B
In general:
2 2 2drift
q
B qB qB
E B E B F Bv
Maxwell’s equations
0 B
t
B
E
0 0 0 t
E
B j
Gauss’ law
No magnetic monopoles
Faraday’s law
Ampére’s law
Lorentz’ force equation
( )q F E v B
Ohm’s law
j E
j
yx zAA A
x y z
A
, ,y yx xz zA AA AA A
y z z x x y
A
Energy density2 2
00
,2 2B E
B EW W
0
E
EF2245 Space Physics 2010
Frozen in magnetic flux PROOF II
2
0
1
t
B
v B B
A B
Order of magnitude estimate:
0
22
0 0
1 m
v BA L vL R
BBL
v B
B
Magnetic Reynolds number Rm:
Rm >> 1 t
B
v B
2
0
1
t
B
BRm << 1
Frozen-in fields!
Diffusion equation!
EF2245 Space Physics 2010
This together with mass conservation, two of Maxwell’s equations and Ohm’s law make up the most common MHD equations:
Magnetohydrodynamics (MHD)
dp
dt
pt
vj B f
vv v j B f (1) ( ) j E v B(3)
0 0 t
EB j(4)
Only consider slow variations
t
B
E(5)
EF2245 Space Physics 2010
v
0t
v(2)
Magnetohydrodynamics (MHD)
dp
dt
vj B(1)
In equilibrium:
0 p j B
0
10p
B B
2
0 0
10
2
Bp
B B
Represents tension along B
If magnetic tension = 0
2
02
Bp konst
Magnetic pressure
EF2245 Space Physics 2010
Solar wind
EF2245 Space Physics 2010
Solar corona
Solar wind properties
1.4∙10-9
1.4∙10-11
1.4∙10-13
1.4∙10-15
Pinterstellar 10-13 – 10-14 Pa
EF2245 Space Physics 2010