Magnetic field lines in ideal turbulent plasmas tend to become quite compli
cated and their length to grow in time. Diffusivity allows for reconnection
and possible shortening, but this fact has not so far been rigorously quan
tified. We show that in a two-dimensional diffusive plasma the mean length
of field lines stays bounded for all time. Moreover, these estimates are lo
cal, in the sense that the mean values of magnetic field and velocity in th
e neighborhood of a ball determine bounds for length within the ball, witho
ut recourse to external magnitudes.