Size: 2142
Comment:
|
Size: 2236
Comment:
|
Deletions are marked like this. | Additions are marked like this. |
Line 35: | Line 35: |
'''Not right ...''' | '''Not right ... we need to integrate from the smallest (but not zero) angle, set by atomic radius perhaps ???''' |
Diffusion
Diffusion turns curvatures in distributions into changes in time. The effect on a point on a curve is to take a little away from the point, and add a little from what is on both sides of it. This can be expressed as
Where F(x,t) is a function in space and time and d is the diffusion constant.
As a difference equation, this can be reformulated as:
So, what is D? Let's figure it out for Rutherford diffusion.
Assume a band of N thinsat atoms occupying a magnetic equatorial band ( B = 90° ) between magnetic radius L and L + d L . Each atom adds a scattering area of:
For small \theta :
This is in all directions. For diffusion that changes the pitch angle \alpha , we need to look at the component in the direction of the field lines only. That will be an annular ring, radius \theta , width d \theta , solid area 2 \pi \theta d \theta .
Let d \alpha = \cos( \gamma ) d \theta . The contribution to the diffusion is proportional to the integral of {\alpha}^2 over the circle:
The area amount d \sigma is multiplied by d N and divided by the area 2 \pi L d L to make d D .
Not right ... we need to integrate from the smallest (but not zero) angle, set by atomic radius perhaps ???