Abstract
Positive Column in magnetic fields B which are much stronger than the critical field Bc for helical instability is studied theoretically. Radial density distributions n0(r) of charged particles are expressed by the confluent hypergeometric function when the time average 〈n1E1〉 is proportional to rn0(r), where n1 and E1 are the fluctuating densities and electric fields. Relative magnitudes of the discharge electric field E0z to that at B=0 are estimated through the degree of 〈n1E1〉. From constant fields E0z regardless of an increase of B, it is derived that |〈n1E1〉| almost linearly depends on B and loss flows of the plasma across B become constant.