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In
plasma physics Plasma ()πλάσμα
, Henry George Liddell, R ...
, Woltjer's theorem states that
force-free magnetic field A force-free magnetic field is a magnetic field in which the Lorentz force is equal to zero and the magnetic pressure greatly exceeds the plasma pressure such that non-magnetic forces can be neglected. For a force-free field, the electric curr ...
s in a closed system with constant force-free parameter \alpha represent the state with lowest magnetic energy in the system and that the
magnetic helicity In plasma physics, magnetic helicity is a measure of the linkage, twist, and writhe of a magnetic field. In ideal magnetohydrodynamics, magnetic helicity is conserved. When a magnetic field contains magnetic helicity, it tends to form large-scal ...
is invariant under this condition. It is named after Lodewijk Woltjer who derived it in 1958.Kholodenko, A. L. (2013). Applications of contact geometry and topology in physics. World Scientific. The force-free field strength \mathbf equation is :\nabla \times \mathbf = \alpha \mathbf. The helicity \mathcal invariant is given by :\frac =0. where \mathcal is related to \mathbf=\nabla\times \mathbf through the
vector potential In vector calculus, a vector potential is a vector field whose curl is a given vector field. This is analogous to a '' scalar potential'', which is a scalar field whose gradient is a given vector field. Formally, given a vector field v, a ''ve ...
\mathbf as below :\mathcal = \int_V \mathbf\cdot\mathbf\ dV = \int_V \mathbf \cdot (\nabla \times \mathbf) \ dV.


See also

*
Chandrasekhar–Kendall function Chandrasekhar–Kendall functions are the axisymmetric eigenfunctions of the curl operator derived by Subrahmanyan Chandrasekhar and P. C. Kendall in 1957 while attempting to solve the force-free magnetic fields. The functions were independently d ...
* Hydrodynamical helicity


References

Astrophysics Plasma physics {{plasma-stub