Test the grad-B drift against the exact orbit

PHYSICS · Multi-part · Fermi University Physics · Computational Physics · Plasma Physics · The plasma state and single-particle motion

Plasma Physics, Ch One particle in given fields: gyration and the guiding-centre drifts

Problem

Test the grad-B drift against the exact orbit. A proton moves in the field B=B0(1+y/L)z^\mathbf{B} = B_0(1 + y/L)\hat{\mathbf{z}} with no electric field. Work in units with q=m=B0=1q = m = B_0 = 1 and initial speed v⊥=1v_\perp = 1, so that time is measured in units of 1/Ω01/\Omega_0 and length in units of rL0=v⊥/Ω0r_{L0} = v_\perp/\Omega_0. Start the proton at (x,y)=(1,0)(x, y) = (1, 0) with velocity (vx,vy)=(0,−1)(v_x, v_y) = (0, -1) and no velocity along zz; its guiding centre then starts at the origin, on the line y=0y = 0 where B=B0B = B_0. Follow the guiding centre through X=x+vy/(1+y/L)X = x + v_y/(1 + y/L), which removes the fast circle from xx. ((a)) Use the grad-B drift to predict the guiding-centre velocity, magnitude and direction, as a function of LL. ((b)) Integrate v˙=v×B\dot{\mathbf{v}} = \mathbf{v}\times\mathbf{B} numerically for L=20L = 20 over 0≤t≤40π0 \le t \le 40\pi, twenty gyroperiods at B0B_0. Find the ratio of the measured drift [X(40π)−X(0)]/40π[X(40\pi) - X(0)]/40\pi to the prediction of part (a). ((c)) Repeat part (b) for L=5L = 5, and explain why the agreement is worse.

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