The linear stability of an array of a large number of thin wires is conside
red. The wires form a cylindrical surface, accelerated toward the axis unde
r the action of a current. Stability equations are derived and a complete c
lassification of the modes is presented. In agreement with Felber and Rosto
ker [Phys. Fluids 24, 1049 (1981)], it is shown that there exist two types
of modes: medial modes, with deformation in the rz plane, and lateral modes
, with only azimuthal deformation. For a given axial wave number, k, the mo
st unstable medial mode has all the wires moving in phase similar to an axi
symmetric mode for a continuous shell, whereas the most unstable lateral pe
rturbation has opposite displacements of neighboring wires. Lateral modes a
re of particular interest because they may remain unstable for parameters w
here medial modes are stable. Numerical analysis of the dispersion relation
for a broad range of modes is presented. Some limiting cases are discussed
. It is shown that k(1/2) scaling holds until surprisingly high wave number
s, even exceeding the inverse interwire distance. In the long-wavelength li
mit, the wires behave as a continuous shell with strong anisotropy of the e
lectrical conductivity, i.e., high along the wires and vanishing across the
wires. The results differ considerably from the modes of a thin, perfectly
conducting shell. In particular, a new "zonal flow" mode is identified. [S
1070-664X(99)01708-5].