A Brief Introduction to Space Plasma Physics.pdf - Institute of ...
A Brief Introduction to Space Plasma Physics.pdf - Institute of ... A Brief Introduction to Space Plasma Physics.pdf - Institute of ...
– For a plane wave solution – The dispersion relationship between the frequency ( ) and the propagation vector ( ) becomes This came from replacing derivatives in time and space by – Case 1 r r r r r u r ~ exp[ i( k r ⋅ −ω t)] ω k r r r r r r r r r r r k )[( C ⋅ k ) u − ( C ⋅u) k − ( k ⋅u C ] = 0 2 2 2 − ω u + ( Cs + CA)( k ⋅u) k + ( CA ⋅ A A ) A k r ⊥ r B 0 2 r ω u ∂ → −iω ∂t r ∇ → ik r ∇⋅ → ik ⋅ r ∇× → ik × = ( C 2 s + C 2 A r r r )( k ⋅u) k
• The fluid velocity must be along k r and perpendicular to 0 B r 0 k r u r • These are magnetosonic waves – Case 2 ( k B r r 1 2 2 v ph = k ( ω ) = ± ( C s+ C k k r B r 0 2 2 2 r r 2 2 2 r r CA −ω ) u + (( Cs CA) −1) k ( CA ⋅u) CA = 0 r • A longitudinal mode with u k r with dispersion relationship ω k (sound waves) r • A transverse mode with k ⋅u r ω = 0 and = ± C A (Alfvén waves) k 2 A ) = ± C s
- Page 5 and 6: - Galileo theorized that aurora is
- Page 7 and 8: The Plasma State • A plasma is an
- Page 9 and 10: • B acts to change the motion of
- Page 11: • The electric field can modify t
- Page 14 and 15: • The change in the direction of
- Page 16 and 17: • Maxwell’s equations - Poisson
- Page 18 and 19: • Maxwell’s equations in integr
- Page 20 and 21: • For a coordinate in which the m
- Page 22 and 23: B r • The force is along and away
- Page 24: - As particles bounce they will dri
- Page 27 and 28: The Properties of a Plasma • A pl
- Page 29 and 30: • For monatomic particles in equi
- Page 31 and 32: • What makes an ionized gas a pla
- Page 34 and 35: • The plasma frequency - Consider
- Page 36 and 37: • A note on conservation laws - C
- Page 38 and 39: - Momentum equation r ∂us r r r r
- Page 40 and 41: • Energy equation ∂ ( ∂t 1 2
- Page 43 and 44: - Often the last terms on the right
- Page 45 and 46: F B • Magnetic pressure and tensi
- Page 47 and 48: •Some elementary wave concepts -F
- Page 49 and 50: • When the dispersion relation sh
- Page 51 and 52: - Incompressible Alfvén waves •
- Page 53 and 54: 1 2 2 C ⎛ B ⎞ A ⎜ ⎟ ⎝ µ
- Page 55: - Continuity - Momentum - Equation
- Page 59: - Arbitrary angle between k r and B
– For a plane wave solution<br />
– The dispersion relationship between the frequency ( ) and<br />
the propagation vec<strong>to</strong>r ( ) becomes<br />
This came from replacing derivatives in time and space by<br />
– Case 1<br />
r<br />
r<br />
r<br />
r<br />
r<br />
u<br />
r<br />
~ exp[ i(<br />
k<br />
r ⋅ −ω<br />
t)]<br />
ω<br />
k r r r r r r r r r r r<br />
k )[( C ⋅ k ) u − ( C ⋅u)<br />
k − ( k ⋅u<br />
C ] = 0<br />
2 2 2<br />
− ω u + ( Cs<br />
+ CA)(<br />
k ⋅u)<br />
k + ( CA<br />
⋅<br />
A<br />
A<br />
)<br />
A<br />
k<br />
r ⊥<br />
r<br />
B 0<br />
2 r<br />
ω u<br />
∂<br />
→ −iω<br />
∂t<br />
r<br />
∇ → ik<br />
r<br />
∇⋅ → ik ⋅<br />
r<br />
∇× → ik ×<br />
= ( C<br />
2<br />
s<br />
+<br />
C<br />
2<br />
A<br />
r r r<br />
)( k ⋅u)<br />
k