Ballooning instability is a phenomenon primarily observed in magnetically confined plasma, typically in the context of nuclear fusion research, specifically in tokamaks and stellarators. It refers to a type of instability that can arise in plasma due to pressure gradients and magnetic field topology. In a magnetic confinement system, plasma is held in place by magnetic fields, which are designed to keep the charged particles (ions and electrons) from escaping.
Articles by others on the same topic
There are currently no matching articles.