- #1
vibe3
- 46
- 1
I have a question about the diamagnetic current caused by plasma pressure gradients. Various plasma physics / MHD texts state that the current due to a plasma pressure gradient in a magnetic field is given by
[tex]\mathbf{J} = \frac{\mathbf{B} \times \nabla p}{B^2}[/tex]
where [tex]p = nkT[/tex]
My question is, if I start with an ambient field [tex]\mathbf{B_0}[/tex] and some density distribution [tex]n(\mathbf{r})[/tex], and I want to calculate this current, can I simply plug in [tex]B_0[/tex] into the equation? Because once the current is flowing, it will change the ambient field into: [tex]B = B_0 + B_1[/tex], where [tex]B_1[/tex] is some additional field due to the current.
How could one account for this and compute the current once steady state has been reached?
[tex]\mathbf{J} = \frac{\mathbf{B} \times \nabla p}{B^2}[/tex]
where [tex]p = nkT[/tex]
My question is, if I start with an ambient field [tex]\mathbf{B_0}[/tex] and some density distribution [tex]n(\mathbf{r})[/tex], and I want to calculate this current, can I simply plug in [tex]B_0[/tex] into the equation? Because once the current is flowing, it will change the ambient field into: [tex]B = B_0 + B_1[/tex], where [tex]B_1[/tex] is some additional field due to the current.
How could one account for this and compute the current once steady state has been reached?
Last edited: