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Magnetic Confinement Fusion - Two stream instability 1 Consider two beams of electrons, each with density n0 , travelling in opposite directions with velocity ±v0 through a background of cold (stationary) ions of density 2n0 . In equilibrium there is no net charge, no current and no magnetic field. The beams are wide enough that the only important direction is parallel to the beams (x). This problem tests the stability of this situation to electrostatic perturbations by treating each electron beam as a fluid: ∂np,m + vp,m · ∇np,m = −np,m ∇ · vp,m ∂t ! me ∂vp,m + vp,m · ∇p,m vp,m ∂t = −eE where the p, m subscripts refer to the fluid with initial velocity plus and minus v0 . 1. Linearise these equations with a perturbation of the form exp (−iωt + ikx), and show that the velocity perturbation is given by ṽp,m = − e2 (ñp + ñm ) / (±kv0 − ω) kme 0 2. By substituting in expressions for ñp and ñm , show that e2 n0 1 1 1= 2 + me 0 (kv0 − ω) (kv0 + ω)2 " # Hint: write vm = −vp (kv0 − ω) / (kv0 + ω) 3. What happens when v0 = 0? 4. Assuming ω 2 is real, find the range of k which is unstable by considering when ω 2 = 0.