Hydrogen-Bonded Liquids 1991
DOI: 10.1007/978-94-011-3274-9_6
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Thermodynamic Properties of Some H-Bonded Liquids in their Undercooled and/or Overcompressed States

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Cited by 4 publications
(2 citation statements)
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“…( 1) and eq. ( 3) gives α P /|α τ | = α P d ln(e(ρ)) d ln(ρ) T τ , which in the case of a power law behavior e(ρ) = ρ x simply reduces to α P • x • T τ , where both α P and T τ depend on P ; usually α P decreases with P [16] and T τ increases with P , leading to a variety of behaviors for α P /|α τ | (see above).…”
Section: Below)mentioning
confidence: 99%
“…( 1) and eq. ( 3) gives α P /|α τ | = α P d ln(e(ρ)) d ln(ρ) T τ , which in the case of a power law behavior e(ρ) = ρ x simply reduces to α P • x • T τ , where both α P and T τ depend on P ; usually α P decreases with P [16] and T τ increases with P , leading to a variety of behaviors for α P /|α τ | (see above).…”
Section: Below)mentioning
confidence: 99%
“…(No data either are available for the pressure dependence of these jumps.) For other molecular glassforming liquids, one observes that the heat capacity C P of the liquid at T g slightly increases with pressure: a few % for 3-methylpentane and 1-propanol up to 200 MPa [34], a few % for m-fluoroaniline up to 400 MPa [35], and 10 − 12 % for toluene up to 400 MPa [36]. However, the C P of the glass at T g has been found to also increase in 3-methylpentane and 1-propanol where it has been measured [34], so that the heat capacity jump ∆C P,g (P) barely changes with pressure in these systems.…”
Section: B Thermodynamic Datamentioning
confidence: 99%