Collisionless plasmas in the solar wind exhibit multi‑scale coupling between microscopic particle kinetics and macroscopic magnetic structure. Although the Vlasov–Maxwell equations fully describe this system, their high dimensionality and non‑linear feedbacks make direct integration impractical for operational forecasting. Traditional fluid closures often fail near instability thresholds, where anisotropy‑driven wave growth rapidly modifies the particle distribution.
Cline SR Carl Dean (Thu,) studied this question.