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Some more thoughts on magnetic ring evolution
I will start with a definition of ram pressure for a cylindrical flow
P_{ram}(r)=\rho_0 (r_o/r)^2 c^2
where r_0 is the initial radius of the cylinder, \rho_0 is the post-shock density in the cylinder and c is the post-shock sound speed.
To get the field that is being stretched by the flow we use flux freezing
B_0 S_0 = B_1 S_1
where S refers to the area the flux threads.
This gives us
B_0 \pi r_0 \delta r_0 = B_1 \pi r_1 \delta r_1
If we now use the tension "pressure" going as
P_t = \frac{B(r)^2}{r}
then we have ram pressure = magnetic tension leading to
B_0^2 r_0^2 r^{-3} = \rho_0 (r_o/r)^2 c^2
or the balance radius r_b
r_b^3 = (\frac{B_0^2 r_0}{\rho_0 c^2})^{1/2}
- Posted: 9 years ago (Updated: 9 years ago)
- Author: Jonathan
- Categories: (none)
Comments
Ahhhh yes flux freezing. That was what i was missing.
So we have
B_o S_o = B_1 S_1
Where S is the area of the annulus through which the field threads which in this case is a ring of thicjness \delta r. The field here is B_x running in the direction of the cylinders axis.
So S = \pi r \delta r
Right?
yea… S_1=\pi r \delta r and S_0 would be the area originally threaded by the ambient field now swept up by the expanding shell . S_0 = \pi (r2 - r02).