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Volumn 57, Issue 1, 1998, Pages 705-719

Frequency-dependent shear viscosity, sound velocity, and sound attenuation near the critical point in liquids. II. Comparison with experiment

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Indexed keywords


EID: 0001278378     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.57.705     Document Type: Article
Times cited : (46)

References (51)
  • 12
    • 85037178517 scopus 로고    scopus 로고
    • L.Ts. Adzhemyan, A.N. Vasiljev, and A.V. Serdukov, in Proceedings of the RG96-Conference, Dubna, August 1996 (World Scientific, Singapore, in press)
    • L.Ts. Adzhemyan, A.N. Vasiljev, and A.V. Serdukov, in Proceedings of the RG96-Conference, Dubna, August 1996 (World Scientific, Singapore, in press).
  • 19
    • 85037254348 scopus 로고    scopus 로고
    • If in the background the correlation length reaches its constant value [Formula Presented] the matching condition leads to a flow parameter depending only on frequency. A simple approximation for not too large frequencies would be [Formula Presented], [Formula Presented]
    • If in the background the correlation length reaches its constant value ξb the matching condition leads to a flow parameter depending only on frequency. A simple approximation for not too large frequencies would be (formula presented).
  • 23
    • 0001258298 scopus 로고
    • the second reference a fit with [Formula Presented] and correction terms is performed. PRBMDO
    • C. Pittman, T. Dorion, and H. Meyer, Phys. Rev. B 20, 3678 (1979). In the second reference a fit with γ=1.24 and correction terms is performed
    • (1979) Phys. Rev. B , vol.20 , pp. 3678
    • Pittman, C.1    Dorion, T.2    Meyer, H.3
  • 25
    • 85037248153 scopus 로고    scopus 로고
    • Note that we use the effective exponent [Formula Presented] instead of [Formula Presented] as in c20, which leads to a different value of [Formula Presented]
    • Note that we use the effective exponent γ=1.19 instead of γ=1.16 as in 20, which leads to a different value of ΓT.
  • 44
    • 85037235972 scopus 로고    scopus 로고
    • (private communication)
    • H. Meyer (private communication).
    • Meyer, H.1
  • 47
    • 85037237105 scopus 로고    scopus 로고
    • c31 [see Fig. 1(c) there] the attenuation has been normalized at each frequency separately. Therefore the agreement at higher frequencies in Fig. 99 is “less perfect” than in the earlier presentation
    • In 31 [see Fig. 1(c) there] the attenuation has been normalized at each frequency separately. Therefore the agreement at higher frequencies in Fig. 99 is “less perfect” than in the earlier presentation.
  • 50
    • 85037214512 scopus 로고    scopus 로고
    • fact one should replot the sound data with the correct nonasymptotic frequency scale. We do not expect substantial changes compared with those presented in Fig. 1515
    • In fact one should replot the sound data with the correct nonasymptotic frequency scale. We do not expect substantial changes compared with those presented in Fig. 1515.


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