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Journal Abstract Search

191 related items for PubMed ID: 16497057

  • 1. Limitations of the rigid planar nonpolarizable models of water.
    Baranyai A, Bartók A, Chialvo AA.
    J Chem Phys; 2006 Feb 21; 124(7):74507. PubMed ID: 16497057
    [Abstract] [Full Text] [Related]

  • 2. Vapor-liquid equilibria from the triple point up to the critical point for the new generation of TIP4P-like models: TIP4P/Ew, TIP4P/2005, and TIP4P/ice.
    Vega C, Abascal JL, Nezbeda I.
    J Chem Phys; 2006 Jul 21; 125(3):34503. PubMed ID: 16863358
    [Abstract] [Full Text] [Related]

  • 3. Characterization of the TIP4P-Ew water model: vapor pressure and boiling point.
    Horn HW, Swope WC, Pitera JW.
    J Chem Phys; 2005 Nov 15; 123(19):194504. PubMed ID: 16321097
    [Abstract] [Full Text] [Related]

  • 4. Clusters of classical water models.
    Kiss PT, Baranyai A.
    J Chem Phys; 2009 Nov 28; 131(20):204310. PubMed ID: 19947683
    [Abstract] [Full Text] [Related]

  • 5. The melting temperature of the most common models of water.
    Vega C, Sanz E, Abascal JL.
    J Chem Phys; 2005 Mar 15; 122(11):114507. PubMed ID: 15836229
    [Abstract] [Full Text] [Related]

  • 6. Computer simulation of two new solid phases of water: Ice XIII and ice XIV.
    Martin-Conde M, MacDowell LG, Vega C.
    J Chem Phys; 2006 Sep 21; 125(11):116101. PubMed ID: 16999507
    [Abstract] [Full Text] [Related]

  • 7. Surface tension of the most popular models of water by using the test-area simulation method.
    Vega C, de Miguel E.
    J Chem Phys; 2007 Apr 21; 126(15):154707. PubMed ID: 17461659
    [Abstract] [Full Text] [Related]

  • 8. Plastic crystal phases of simple water models.
    Aragones JL, Vega C.
    J Chem Phys; 2009 Jun 28; 130(24):244504. PubMed ID: 19566163
    [Abstract] [Full Text] [Related]

  • 9. Dielectric constant of ices and water: a lesson about water interactions.
    Aragones JL, MacDowell LG, Vega C.
    J Phys Chem A; 2011 Jun 16; 115(23):5745-58. PubMed ID: 20866096
    [Abstract] [Full Text] [Related]

  • 10. The short range anion-H interaction is the driving force for crystal formation of ions in water.
    Alejandre J, Chapela GA, Bresme F, Hansen JP.
    J Chem Phys; 2009 May 07; 130(17):174505. PubMed ID: 19425788
    [Abstract] [Full Text] [Related]

  • 11. Properties of ices at 0 K: a test of water models.
    Aragones JL, Noya EG, Abascal JL, Vega C.
    J Chem Phys; 2007 Oct 21; 127(15):154518. PubMed ID: 17949184
    [Abstract] [Full Text] [Related]

  • 12. Liquid-liquid phase transitions in supercooled water studied by computer simulations of various water models.
    Brovchenko I, Geiger A, Oleinikova A.
    J Chem Phys; 2005 Jul 22; 123(4):044515. PubMed ID: 16095377
    [Abstract] [Full Text] [Related]

  • 13. Simulating vapor-liquid nucleation of water: A combined histogram-reweighting and aggregation-volume-bias Monte Carlo investigation for fixed-charge and polarizable models.
    Chen B, Siepmann JI, Klein ML.
    J Phys Chem A; 2005 Feb 17; 109(6):1137-45. PubMed ID: 16833423
    [Abstract] [Full Text] [Related]

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  • 16. The melting point of ice Ih for common water models calculated from direct coexistence of the solid-liquid interface.
    García Fernández R, Abascal JL, Vega C.
    J Chem Phys; 2006 Apr 14; 124(14):144506. PubMed ID: 16626213
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  • 18. Relation between the melting temperature and the temperature of maximum density for the most common models of water.
    Vega C, Abascal JL.
    J Chem Phys; 2005 Oct 08; 123(14):144504. PubMed ID: 16238404
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  • 20. Capillary waves at the liquid-vapor interface and the surface tension of water.
    Ismail AE, Grest GS, Stevens MJ.
    J Chem Phys; 2006 Jul 07; 125(1):014702. PubMed ID: 16863319
    [Abstract] [Full Text] [Related]

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