Showing posts with label Guiding center positions. Show all posts
Showing posts with label Guiding center positions. Show all posts

Monday, January 11, 2016

Solutions to Space Plasma Physics Problems (1)


1)      Find the ion and electron gyrofrequencies for an ion and electron in solar plasma with a magnetic induction (field strength) of B = 0.0001 T.

Solution:   The ion gyrofrequency will be:

i  = qB/ m i  =   [(1.6 x 10 -19  C) (0.0001 T) ]/ 1.7 x 10 -27  kg
i   =  9.4 x 10 3 /s

 And the electron gyrofrequency is:

 e  = qB/ m e  =   [(1.6 x 10 -19  C) (0.0001 T) ]/ 9.1 x 10 -31  kg

e  =  1.7 x 10 7  /s


2)     If the perpendicular velocity component ( v) is 105  m/s for the electron, find its Larmor radius and its gyro-period.

 
Larmor radius:  r = m/ q [v / B] =  v/ (qB/ m e) = v/ e

 r = (10 5  m/s) / 1.7 x 10 7  /s   =     0.0056 m or:  0.56 cm

Gyro-period: T = 2 p  / e  =   2 p / 1.7 x 10 7  /s   =  3.5 x 10 -7  s

3)     Thence or otherwise obtain the gyration energy in eV.
(1.6 x 10 -19  J = 1 eV)

 Gyration energy E = m e  (v)2/ 2 =  
  (9.1 x 10 -31  kg) (10 5  m/s) 2  / 2

E =    4.5 x 10 -21  J  Or: in Electron volts:  
 
 (4.5 x 10 -21  J )/ (1.6 x 10 -19  J/eV) = 0.028 eV


4)     Find the guiding center positions for the electron referenced above (previous problems) if t = T/4.

 Guiding center positions:

 x – xo =   r sin (e t)   =    (0.0056 m)  sin (e  T/4) = 

=  (0.0056 m) sin [(1.7 x 10 7  /s) (3.5 x 10 -7  s/ 4)] = 0.0056 m

y – yo =   r cos (e t)   =    
(0.0056 m) sin [(1.7 x 10 7  /s) (3.5 x 10 -7  s/ 4)] = 0

 To see how these values can be, note that: (e T)   = 6.28 rad = 2p rad

 So:  (e T/ 4)   =1.57 rad =  p  / 2

 But:  sin (p /2) = 1 and (cos p /2) = 0

 So the value for x – xo is simply dictated by the value for  r

 5) What other critical information do you need to obtain the E-field at the guiding center?

From the information provided we see that:

v d     = (1 +    ¼ r 2  v2 ) o  X B/  B 2

 So the other information needed to obtain o  would be the drift velocity, v d  .