TY - JOUR
T1 - Evidence of low-density and high-density liquid phases and isochore end point for water confined to carbon nanotube
AU - Nomura, Kentaro
AU - Kaneko, Toshihiro
AU - Bai, Jaeil
AU - Francisco, Joseph S.
AU - Yasuoka, Kenji
AU - Zeng, Xiao Cheng
PY - 2017/4/18
Y1 - 2017/4/18
N2 - 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.
AB - 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.
KW - Confined water
KW - Free energy surface
KW - High-density liquid
KW - Low-density liquid
KW - Molecular dynamics simulation
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U2 - 10.1073/pnas.1701609114
DO - 10.1073/pnas.1701609114
M3 - Article
C2 - 28373562
AN - SCOPUS:85017585535
SN - 0027-8424
VL - 114
SP - 4066
EP - 4071
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 16
ER -