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The analysis of in situ plasma electron observations in the Io plasma torus by the plasma science experiment during the Voyager 1 encounter with Jupiter is presented in terms of two components: a thermal ( c ) Maxwellian component and suprathermal ( H ) non‐Maxwellian component of the electron distribution function. Average electron temperatures are T e 7.6) and then continues to rise to T e > 100 eV at r > 12 R J . In the cold torus the density ratio of the suprathermal component n H to that of the cold component n c was 2.5 µV/m which exceeds the ambipolar electric field E ∥ < 1 µV/m produced by the centrifugally confined ions. However, if unacceptable charge imbalances in the thermal plasma are not to occur from this larger E ∥ , then sufficient wave turbulence in the plasma must be present to adequately scatter the thermal electrons. We infer the presence of a neutral corona around Io from the observed decrease and symmetry with respect to Io of T c . The energy input to the torus by charge exchange and ionization in this neutral corona followed by pickup is ∼2 × 10 11 W, substantially less than the EUV luminosity. In the hot torus, suprathermal electrons contribute significantly to the ionization of the more highly ionized ions (O + , O 2+ , S 2+ , and S 3+ ).
Sittler et al. (Mon,) studied this question.
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