Now, the magnitude of the associated B-field before the shock is obtained via:
Ω e = qB/
m e
So: B = Ω e m e / q
= (1.9 x 10 7 /s
) (9.1 x 10 -31
kg)/ (1.6 x 10 -19 C)
= 10 -4 T
This is the equilibrium value of B before the shock is applied. But from the shock equation:
B m = (2M – 1) Bo = (2(80) – 1) 10 -4 T = 0.015 T
Which is the magnetic field associated with the collisionless shock.
2)The pure electron plasma frequency is:
n =
9 Ö N = 9 Ö (10
16 /m3) = 9 x 10 8
/s
Then: we = 2p
n = 2p(9 x 10 8 /s ) = 5.6 x 10 9 /s
Debye length l D, =
[(1.38 x 10-23
)(10 6K) (8.85 x 10 -12 F/m) / (4p) (10 16/m3) e2 ]
½
= 1.9 x 10 - 4 m
Plasma parameter: L = n o
l3 D
= ( 10 16
/m3) (1.9 x 10 -
4 m) 3
L = 7.4
x 10 4
The
radio emission must exceed this
900 MHz frequency for propagation in the medium, so we need:
f
> 9 x 10 8 Hz = 900 MHz
we = 2p (9 x 10 8 /s )
= 5.6 x 10 9 /s
k
w = we/ u » (5.6 x 10 9
/s )/ 10 5 m/ s
k
w = 5.6
x 10 4 m-1
4) We need to re-arrange the equation to solve for velocity v o:
Using
algebra we find:
v o = w/ k w - 1/
k w [1/(wp 2 - (m/M)/ w2] 1/2
Substitute values: v o =
(10 10 s-1 )/
5.6 x 10 4 m-1 -
1/(5.6 x 10 4
m-1) [1/(5.6 x 10 9
s-1) 2 - (5.4 x 10 4
)/ (10 10 s-1) 2] 1/2
v o = 7.8 x 10 4
ms-1
5) The shock equation is:
B m = (2M – 1) Bo
We can estimate the value of M from the ratio of the velocities: u/ v
Where u/ v = (10 5 ms-1) / ( 7.8 x 10 4 ms-1 ) » 1.3
Then: B m = (2M – 1) Bo » (2(1.3) -1 ) Bo » (2.6 - 1) Bo » 1.6 Bo
6) The
form of the result yields 9 as a constant outside the root sign so we must
have:
9 » e/2p Ö( 1 / εo m
e )
Compute:
e/2p Ö( 1 / εo m
e ) =
1.6
x 10 - 19 C/ 2p Ö( 1 / (8.5 x
10 -12 F/m)( 9.1 x 10 - 31 kg)
= 8.973 Ö N or n »
9 Ö N
No comments:
Post a Comment