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76 v (z) = c”(a+z)-m, where a, cV and m are constants. The transversal distribution followed the known exponential relation. With equation 5 we get IO = IO- $-r. $.Cv . (l+z)_” [kl I where k1 = normalizing factor. I,, represents the current flowing off between z = 0 and z. Figure 4 shows the increase of ID and the decrease of Iz with z for those jets as in figure 3. If I,, flows steadily through the conical jet (7) surface a mean drift current density j, = O.ZOnA/cm* respectively 0.15nA/cmZ follows from figure 4. Y- Experimental measurements gave J,, = (0.2.. .0.5)nA/cmZ. J01 J02 To = 0123L567 lengthz, m Fig.4. Calculated drift currents I,, and the corresponding current the jet axis, expansion conditions as in fig.3. Iz along The measurements of the drift currents close to the jet are influenced by field distortions and discharges. Therefore only the range of measured values is given. The drift current starts at the jet boundary and its magnitude also depends on the difference between the actual and the saturation vapour pressure of water in the ambient air. A strong reduction of ID takes place if the relative humidity reaches values of greater than 95 per cent. This is connected with an increasing “electrical” jet length and a reduced decay of thePDF Image | ELECTROSTATIC EFFECTS OF CHARGED STEAM JETS
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