TY - JOUR
T1 - Size-dependent phase changes in water clusters
AU - Kaneko, Toshihiro
AU - Akimoto, Takuma
AU - Yasuoka, Kenji
AU - Mitsutake, Ayori
AU - Zeng, Xiao Cheng
PY - 2011/10/11
Y1 - 2011/10/11
N2 - We investigate melting behavior of water clusters (H2O) N (N = 7, 8, 11, and 12) by using multicanonical-ensemble molecular dynamics simulations. Our simulations show that the melting behavior of water clusters is highly size dependent. Based on the computed canonical average of the potential energy and heat capacity CV, we conclude that (H 2O)8 and (H2O)12 exhibit first-order-like phase change, while (H2O)7 and (H 2O)11 exhibit continuous-like phase change. The melting temperature range for (H2O)8 and (H2O) 12 can be defined based on the peak position of CV(T) and dCV(T)/dT (where T is the temperature). Moreover, for (H 2O)8 and (H2O)12, the solid- and liquid-like phases separate temporally in the course of simulation. In contrast, no temporal separation of solid- and liquid-like phases is observed for (H 2O)7 and (H2O)11. In light of the notable temporal separation of solid- and liquid-like phases for(H 2O)8 and (H2O)12, an alternative computer approach for estimating the melting temperature range is proposed based on the time-dependent Lindemann parameters. We find that the melting temperature range estimated from both definitions is consistent with each other for (H2O)8 and (H2O)12 but not for (H2O)7 and (H2O)11. We also find that the melting behavior of small water clusters can be conveniently assessed if the energy differences of neighbor-sized clusters at zero temperature are known.
AB - We investigate melting behavior of water clusters (H2O) N (N = 7, 8, 11, and 12) by using multicanonical-ensemble molecular dynamics simulations. Our simulations show that the melting behavior of water clusters is highly size dependent. Based on the computed canonical average of the potential energy and heat capacity CV, we conclude that (H 2O)8 and (H2O)12 exhibit first-order-like phase change, while (H2O)7 and (H 2O)11 exhibit continuous-like phase change. The melting temperature range for (H2O)8 and (H2O) 12 can be defined based on the peak position of CV(T) and dCV(T)/dT (where T is the temperature). Moreover, for (H 2O)8 and (H2O)12, the solid- and liquid-like phases separate temporally in the course of simulation. In contrast, no temporal separation of solid- and liquid-like phases is observed for (H 2O)7 and (H2O)11. In light of the notable temporal separation of solid- and liquid-like phases for(H 2O)8 and (H2O)12, an alternative computer approach for estimating the melting temperature range is proposed based on the time-dependent Lindemann parameters. We find that the melting temperature range estimated from both definitions is consistent with each other for (H2O)8 and (H2O)12 but not for (H2O)7 and (H2O)11. We also find that the melting behavior of small water clusters can be conveniently assessed if the energy differences of neighbor-sized clusters at zero temperature are known.
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U2 - 10.1021/ct200458m
DO - 10.1021/ct200458m
M3 - Article
AN - SCOPUS:80054005280
SN - 1549-9618
VL - 7
SP - 3083
EP - 3087
JO - Journal of Chemical Theory and Computation
JF - Journal of Chemical Theory and Computation
IS - 10
ER -