Evidence of low-density and high-density liquid phases and isochore end point for water confined to carbon nanotube

被引:43
作者
Nomura, Kentaro [1 ]
Kaneko, Toshihiro [2 ,3 ]
Bai, Jaeil [4 ]
Francisco, Joseph S. [4 ]
Yasuoka, Kenji [1 ]
Zeng, Xiao Cheng [4 ,5 ]
机构
[1] Keio Univ, Dept Mech Engn, Yokohama, Kanagawa 2238522, Japan
[2] Tokyo Univ Sci, Dept Mech Engn, Noda, Chiba 2788510, Japan
[3] Tokyo Univ Sci, Res Inst Sci & Technol, Noda, Chiba 2788510, Japan
[4] Univ Nebraska, Dept Chem, Lincoln, NE 68588 USA
[5] Beijing Univ Chem Technol, Beijing Adv Innovat Ctr Soft Matter Sci & Engn, Beijing 100029, Peoples R China
基金
美国国家科学基金会;
关键词
low-density liquid; high-density liquid; confined water; free energy surface; molecular dynamics simulation; ICE-NANOTUBES; AMORPHOUS ICE; GLASSY WATER; TRANSITION; PRESSURE; BEHAVIOR; DIAGRAM;
D O I
10.1073/pnas.1701609114
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
Possible transition between two phases of supercooled liquid water, namely the low-and high-density liquid water, has been only predicted to occur below 230 K from molecular dynamics (MD) simulation. However, such a phase transition cannot be detected in the laboratory because of the so-called "no-man's land" under deeply supercooled condition, where only crystalline ices have been observed. Here, we show MD simulation evidence that, inside an isolated carbon nanotube (CNT) with a diameter of 1.25 nm, both lowand high-density liquid water states can be detected near ambient temperature and above ambient pressure. In the temperature-pressure phase diagram, the low-and high-density liquid water phases are separated by the hexagonal ice nanotube (hINT) phase, and the melting line terminates at the isochore end point near 292 K because of the retracting melting line from 292 to 278 K. Beyond the isochore end point (292 K), low-and high-density liquid becomes indistinguishable. When the pressure is increased from 10 to 600 MPa along the 280-K isotherm, we observe that water inside the 1.25-nm-diameter CNT can undergo low-density liquid to hINT to high-density liquid reentrant first-order transitions.
引用
收藏
页码:4066 / 4071
页数:6
相关论文
共 36 条
[1]  
Agrawal KV, 2017, NAT NANOTECHNOL, V12, P267, DOI [10.1038/NNANO.2016.254, 10.1038/nnano.2016.254]
[2]   Multiwalled ice helixes and ice nanotubes [J].
Bai, Jaeil ;
Wang, Jun ;
Zeng, X. C. .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2006, 103 (52) :19664-19667
[3]   FINITE-SIZE EFFECTS AT TEMPERATURE-DRIVEN 1ST-ORDER TRANSITIONS [J].
CHALLA, MSS ;
LANDAU, DP ;
BINDER, K .
PHYSICAL REVIEW B, 1986, 34 (03) :1841-1852
[4]   Metastability and no criticality [J].
Chandler, D. .
NATURE, 2016, 531 (7593) :E1-E2
[5]   Supercooled and glassy water [J].
Debenedetti, PG .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2003, 15 (45) :R1669-R1726
[6]   New porous water ice metastable at atmospheric pressure obtained by emptying a hydrogen-filled ice [J].
del Rosso, Leonardo ;
Celli, Milva ;
Ulivi, Lorenzo .
NATURE COMMUNICATIONS, 2016, 7
[7]   Formation and properties of ice XVI obtained by emptying a type sII clathrate hydrate [J].
Falenty, Andrzej ;
Hansen, Thomas C. ;
Kuhs, Werner F. .
NATURE, 2014, 516 (7530) :231-+
[8]   Structure of a new dense amorphous ice [J].
Finney, JL ;
Bowron, DT ;
Soper, AK ;
Loerting, T ;
Mayer, E ;
Hallbrucker, A .
PHYSICAL REVIEW LETTERS, 2002, 89 (20)
[9]   Carbon nanotube flow sensors [J].
Ghosh, S ;
Sood, AK ;
Kumar, N .
SCIENCE, 2003, 299 (5609) :1042-1044
[10]  
Ghosh S, 2004, EUROPHYS LETT, V65, P678, DOI 10.1209/ep1/i2003-10160-9