Glass-liquid transition of water at high pressure
The knowledge of the existence of liquid water under extreme conditions and its concomitant properties are important in many fields of science. Glassy water has previously been prepared by hyperquenching micron-sized droplets of liquid water and vapor deposition on a cold substrate (ASW), and its tr...
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Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2011-07, Vol.108 (27), p.11013-11016 |
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description | The knowledge of the existence of liquid water under extreme conditions and its concomitant properties are important in many fields of science. Glassy water has previously been prepared by hyperquenching micron-sized droplets of liquid water and vapor deposition on a cold substrate (ASW), and its transformation to an ultraviscous liquid form has been reported on heating. A densified amorphous solid form of water, high-density amorphous ice (HDA), has also been made by collapsing the structure of ice at pressures above 1 GPa and temperatures below approximately 140 K, but a corresponding liquid phase has not been detected. Here we report results of heat capacity Cp and thermal conductivity, in situ, measurements, which are consistent with a reversible transition from annealed HDA to ultraviscous high-density liquid water at 1 GPa and 140 K. On heating of HDA, the Cp increases abruptly by (3.4 ± 0.2) J molâ»Â¹ Kâ»Â¹ before crystallization starts at (153 ± 1) K. This is larger than the Cp rise at the glass to liquid transition of annealed ASW at 1 atm, which suggests the existence of liquid water under these extreme conditions. |
doi_str_mv | 10.1073/pnas.1016520108 |
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Glassy water has previously been prepared by hyperquenching micron-sized droplets of liquid water and vapor deposition on a cold substrate (ASW), and its transformation to an ultraviscous liquid form has been reported on heating. A densified amorphous solid form of water, high-density amorphous ice (HDA), has also been made by collapsing the structure of ice at pressures above 1 GPa and temperatures below approximately 140 K, but a corresponding liquid phase has not been detected. Here we report results of heat capacity Cp and thermal conductivity, in situ, measurements, which are consistent with a reversible transition from annealed HDA to ultraviscous high-density liquid water at 1 GPa and 140 K. On heating of HDA, the Cp increases abruptly by (3.4 ± 0.2) J molâ»Â¹ Kâ»Â¹ before crystallization starts at (153 ± 1) K. 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Glassy water has previously been prepared by hyperquenching micron-sized droplets of liquid water and vapor deposition on a cold substrate (ASW), and its transformation to an ultraviscous liquid form has been reported on heating. A densified amorphous solid form of water, high-density amorphous ice (HDA), has also been made by collapsing the structure of ice at pressures above 1 GPa and temperatures below approximately 140 K, but a corresponding liquid phase has not been detected. Here we report results of heat capacity Cp and thermal conductivity, in situ, measurements, which are consistent with a reversible transition from annealed HDA to ultraviscous high-density liquid water at 1 GPa and 140 K. On heating of HDA, the Cp increases abruptly by (3.4 ± 0.2) J molâ»Â¹ Kâ»Â¹ before crystallization starts at (153 ± 1) K. This is larger than the Cp rise at the glass to liquid transition of annealed ASW at 1 atm, which suggests the existence of liquid water under these extreme conditions.</description><subject>Chemical vapor deposition</subject><subject>cold</subject><subject>Cooling</subject><subject>Crystallization</subject><subject>droplets</subject><subject>Glass</subject><subject>glass transition</subject><subject>Glass transition temperature</subject><subject>heat</subject><subject>Heat conductivity</subject><subject>Ice</subject><subject>Kinetics</subject><subject>Liquids</subject><subject>Physical Sciences</subject><subject>pressure-induced amorphization</subject><subject>relaxation</subject><subject>Relaxation time</subject><subject>Specific heat</subject><subject>Substrates</subject><subject>Temperature</subject><subject>thermal conductivity</subject><subject>Transition temperature</subject><subject>water vapor</subject><issn>0027-8424</issn><issn>1091-6490</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>D8T</sourceid><recordid>eNpdkc1v1DAQxS0EosvCmRMQcemF0Bk7_rpUqkopSJU4QLlaTuLd9Sobb-2Eiv8eR1m6FPlgS-83b2b8CHmN8BFBsrN9b1N-oeAUENQTskDQWIpKw1OyAKCyVBWtTsiLlLYAoLmC5-SEotDABC4IXnc2pbLzd6NviyHaPvnBh74Iq-LeDi4Wdig2fr0p9tGlNEb3kjxb2S65V4d7SW4_X_24_FLefLv-enlxUzZcs6FkEjl1LVMUkSKv0TYN1pIx3tRMtA1Ao3hNV1RQVXGoNWtaIbngWkklbM2W5MPsm-7dfqzNPvqdjb9NsN588j8vTIhrM-5GU2lWyYyfz3hmd65tXJ-X6R5VPVZ6vzHr8MswzCePvCSnB4MY7kaXBrPzqXFdZ3sXxmSU5JVSuoJMvv-P3IYx9vkzJohTRsU0z9kMNTGkFN3qYRQEM2VnpuzMMbtc8fbfDR74v2FloDgAU-XRThkqDWYnlpE3M7JNQ4hHC6mlkqzK-rtZX9lg7Dr6ZG6_5_YCADXKHM8fn3ixMw</recordid><startdate>20110705</startdate><enddate>20110705</enddate><creator>Andersson, Ove</creator><general>National Academy of Sciences</general><general>National Acad Sciences</general><scope>FBQ</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QG</scope><scope>7QL</scope><scope>7QP</scope><scope>7QR</scope><scope>7SN</scope><scope>7SS</scope><scope>7T5</scope><scope>7TK</scope><scope>7TM</scope><scope>7TO</scope><scope>7U9</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H94</scope><scope>M7N</scope><scope>P64</scope><scope>RC3</scope><scope>7X8</scope><scope>5PM</scope><scope>ADHXS</scope><scope>ADTPV</scope><scope>AOWAS</scope><scope>D8T</scope><scope>D93</scope><scope>ZZAVC</scope></search><sort><creationdate>20110705</creationdate><title>Glass-liquid transition of water at high pressure</title><author>Andersson, Ove</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c593t-37152ed38211215b1acc1b7335cb36dc00c85b2f2628450b93cd6756598786ab3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Chemical vapor deposition</topic><topic>cold</topic><topic>Cooling</topic><topic>Crystallization</topic><topic>droplets</topic><topic>Glass</topic><topic>glass transition</topic><topic>Glass transition temperature</topic><topic>heat</topic><topic>Heat conductivity</topic><topic>Ice</topic><topic>Kinetics</topic><topic>Liquids</topic><topic>Physical Sciences</topic><topic>pressure-induced amorphization</topic><topic>relaxation</topic><topic>Relaxation time</topic><topic>Specific heat</topic><topic>Substrates</topic><topic>Temperature</topic><topic>thermal conductivity</topic><topic>Transition temperature</topic><topic>water vapor</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Andersson, Ove</creatorcontrib><collection>AGRIS</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Animal Behavior Abstracts</collection><collection>Bacteriology Abstracts (Microbiology B)</collection><collection>Calcium & Calcified Tissue Abstracts</collection><collection>Chemoreception Abstracts</collection><collection>Ecology Abstracts</collection><collection>Entomology Abstracts (Full archive)</collection><collection>Immunology Abstracts</collection><collection>Neurosciences Abstracts</collection><collection>Nucleic Acids Abstracts</collection><collection>Oncogenes and Growth Factors Abstracts</collection><collection>Virology and AIDS Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Engineering Research Database</collection><collection>AIDS and Cancer Research Abstracts</collection><collection>Algology Mycology and Protozoology Abstracts (Microbiology C)</collection><collection>Biotechnology and BioEngineering Abstracts</collection><collection>Genetics Abstracts</collection><collection>MEDLINE - 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Glassy water has previously been prepared by hyperquenching micron-sized droplets of liquid water and vapor deposition on a cold substrate (ASW), and its transformation to an ultraviscous liquid form has been reported on heating. A densified amorphous solid form of water, high-density amorphous ice (HDA), has also been made by collapsing the structure of ice at pressures above 1 GPa and temperatures below approximately 140 K, but a corresponding liquid phase has not been detected. Here we report results of heat capacity Cp and thermal conductivity, in situ, measurements, which are consistent with a reversible transition from annealed HDA to ultraviscous high-density liquid water at 1 GPa and 140 K. On heating of HDA, the Cp increases abruptly by (3.4 ± 0.2) J molâ»Â¹ Kâ»Â¹ before crystallization starts at (153 ± 1) K. 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subjects | Chemical vapor deposition cold Cooling Crystallization droplets Glass glass transition Glass transition temperature heat Heat conductivity Ice Kinetics Liquids Physical Sciences pressure-induced amorphization relaxation Relaxation time Specific heat Substrates Temperature thermal conductivity Transition temperature water vapor |
title | Glass-liquid transition of water at high pressure |
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