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Related Concept Videos

Phase Transitions: Melting and Freezing02:39

Phase Transitions: Melting and Freezing

Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
Phase Transitions: Sublimation and Deposition02:33

Phase Transitions: Sublimation and Deposition

Some solids can transition directly into the gaseous state, bypassing the liquid state, via a process known as sublimation. At room temperature and standard pressure, a piece of dry ice (solid CO2) sublimes, appearing to gradually disappear without ever forming any liquid. Snow and ice sublimate at temperatures below the melting point of water, a slow process that may be accelerated by winds and the reduced atmospheric pressures at high altitudes. When solid iodine is warmed, the solid sublimes...
Structures of Solids02:22

Structures of Solids

Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...
Ionic Crystal Structures02:42

Ionic Crystal Structures

Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Chair Conformation of Cyclohexane02:02

Chair Conformation of Cyclohexane

The chair conformation is the most stable form of cyclohexane due to the absence of angle and torsional strain. The absence of angle strain is a result of cyclohexane’s bond angle being very close to the ideal tetrahedral bond angle of 109.5° in its chair conformer. Similarly, the torsional strain is also absent owing to the perfectly staggered arrangement of bonds.
The hydrogen atoms linked to carbons are arranged in two different axial and equatorial orientations to achieve this staggered...
Thermal Sigmatropic Reactions: Overview01:16

Thermal Sigmatropic Reactions: Overview

Sigmatropic rearrangements are a class of pericyclic reactions in which a σ bond migrates from one part of a π system to another. These are intramolecular rearrangements where the total number of σ and π bonds remain unchanged.
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Determining the Ice-binding Planes of Antifreeze Proteins by Fluorescence-based Ice Plane Affinity
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Reversible structure transformation in ice nanocluster.

Kengo Nishio1, Masuhiro Mikami

  • 1Research Institute for Computational Sciences, National Institute of Advanced Industrial Science and Technology, Central 2, Umezono 1-1-1, Tsukuba, Ibaraki 305-8568, Japan. k-nishio@aist.go.jp

The Journal of Chemical Physics
|April 25, 2009
PubMed
Summary

Nanosized water clusters exhibit unique behaviors not seen in bulk ice. Molecular dynamics simulations show that small ice structures dynamically change and coexist in various solid-like phases, even at low temperatures.

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Area of Science:

  • Physical Chemistry
  • Nanotechnology
  • Materials Science

Background:

  • Bulk water freezes into a stable solid phase (ice) upon cooling.
  • Phase transitions in bulk water are well-understood and typically require heating above the melting point to reverse.
  • The behavior of water at the nanoscale can differ significantly from its bulk properties.

Purpose of the Study:

  • To investigate the phase behavior of nanosized water clusters.
  • To explore non-bulk-like phenomena in ice nanoclusters using molecular dynamics.
  • To characterize the structural dynamics and coexisting phases of small water clusters.

Main Methods:

  • Molecular-dynamics simulations were employed.
  • The TIP4P water potential was used for simulations.
  • Simulations were conducted for (H2O)20 nanoclusters over 100 microseconds.

Main Results:

  • Nanosized ice clusters exhibit reversible structural changes.
  • A variety of solid-like phases dynamically coexist within the nanocluster.
  • Observed structures include bilayer prisms, ice nanotubes (square and pentagonal), and fullerene-like cages.
  • These diverse phases exist even at temperatures significantly below the bulk melting point (down to 52%).

Conclusions:

  • Nanoscale ice does not behave like bulk ice, displaying unique structural flexibility.
  • The dynamic coexistence of multiple solid-like phases is a characteristic feature of water nanoclusters.
  • These findings challenge conventional understanding of ice phase behavior at the nanoscale.