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Using observations made by the solar wind ion composition spectrometer on Ulysses during its trip in the ecliptic plane to Jupiter, we examined the temperature ratios T( 4 He 2+ )/T(H + ) and T(O 6+ )/T(H + ) across 15 shocks, including forward and reverse shock pairs as well as isolated shocks. The mean value over the whole set of downstream data studied was 7±3 for the T( 4 He 2+ )/T(H + ). Appreciable differentiated heating downstream of a shock occurred for an upstream ratio T( 4 He 2+ )/T(H + )<4.5. Downstream in the shock regions, characterized by a quasisteady plasma flux, values of T( 4 H 2+ )/T(H + ) and T(O 6+ )/T(H + ) are observed in the range 4.6 to 10.8 and 19 to 48, respectively. Downstream of the shock, extra‐heated ions heavier than H + added a mean 13±6% to the ions' plasma pressure. (This is in addition to the pressure calculated using the common assumption of a temperature scaling with the ion masses in heliospheric collisionless plasma.) The extra heating of 4 He 2+ relative to H + was larger for a smaller plasma β, agreeing with the prediction of the magnetohydrodynamic calculations by Zhao et al . [1991], although they appeared to underestimate the amount of added heating by a factor of 1.25 to 2.
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Berdichevsky et al. (1997) studied this question.
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