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Equation of state of3He near its liquid-vapor critical point
Authors:Robert P Behringer  Ted Doiron  Horst Meyer
Affiliation:(1) Department of Physics, Duke University, Durham, North Carolina;(2) Present address: Bell Laboratories, Murray Hill, New Jersey
Abstract:We report high-resolution measurements of the pressure coefficient (partP/partT)rgr for3He in both the one-phase and two-phase regions close to the critical point. These include data on 40 isochores over the intervals–0.1letle+0.1 and–0.2leDeltargrle+0.2, wheret=(T–T c )/T c and Deltargr=(rgrrgr c )/rgr c . We have determined the discontinuity Delta(partP/partT)rgr of (partP/partT)rgr between the one-phase and the two-phase regions along the coexistence curve as a function of Deltargr. The asymptotic behavior of (1/rgr) Delta(partP/partT)rgr versus Deltargr near the critical point gives a power law with an exponent (gamma+beta–1)beta–1=1.39±0.02 for0.01lEDeltargrle0.2 or–1×10 –2letle10 –6 , from which we deduce gamma=1.14±0.01, using beta=0.361 determined from the shape of the coexistence curve. An analysis of the discontinuity Delta(partP/partT)rgr with a correction-to-scaling term gives gamma=1.17±0.02. The quoted errors are fromstatistics alone. Furthermore, we combine our data with heat capacity results by Brown and Meyer to calculate (partmgr/partT)rgr c as a function oft. In the two-phase region the slope (part2mgr/partT 2)rgrc is different from that in the one-phase region. These findings are discussed in the light of the predictions from simple scaling and more refined theories and model calculations. For the isochores Deltargrne0 we form a scaling plot to test whether the data follow simple scaling, which assumes antisymmetry of mgrmgr (rgr c ,t) as a function of Deltagamma on both sides of the critical isochore. We find that indeed this plot shows that the assumption of simple scaling holds reasonably well for our data over the rangeVerbartVerbarle0.1. A fit of our data to the ldquolinear modelrdquo approximation is obtained forVerbarDeltargrVerbarle0.10 andtle0.02, giving a value of gamma=1.16±0.02. Beyond this range, deviations between the fit and the data are greater than the experimental scatter. Finally we discuss the (partP/partT)rgr data analysis for 4 He by Kierstead. A power law plot of (1/rgr) DeltapartP/partT)rgr versus Deltargr belowT c leads to gamma=1.13±0.10. An analysis with a correction-to-scaling term gives gamma=1.06±0.02. In contrast to 3 He, the slopes (part2mgr/partT 2)rgrc above and belowT c are only marginally different.Work supported by a grant from the National Science Foundation.
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