Magnetic fluctuation induced electron energy transport is measured in
the Continuous Current Tokamak [R.J. Taylor et al., Phys. Rev. Lett. 6
3, 2365 (1989)] at 0.75 < r/a < 1 for fluctuations with 0 < f < 150 kH
z. The flux, produced by electrons traveling parallel to a fluctuating
magnetic field, is obtained from the correlation between the fluctuat
ions in the parallel heat flux and the radial magnetic field. It was f
ound that the magnetic fluctuations do not contribute to the total ene
rgy transport except in the vicinity of the q = 2 magnetic surface in
the presence of large amplitude Mirnov oscillation.