
Phases of ice - Wikipedia
On Earth, most ice is found in the hexagonal Ice I h phase. Less common phases may be found in the atmosphere and underground due to more extreme pressures and temperatures. Some …
冰III - 维基百科,自由的百科全书
冰III,读作“冰三”,是 冰 的一种 晶体 形态,属于 四方晶系,可以将 水 在 300 MPa 下降温到 250 K (-23.15 °C) 制得。 它在所有高压水 相 中是密度最低的,在 350 MPa 下仅 1160 kg/m3。
已知的冰相有多少种?分别有哪些特点? - 知乎
III相:III相也叫低温冰,是在低温下形成的冰相。 III相的分子结构为正十二面体结构,每个氧原子周围有12个氢原子成键,每个氢原子周围有两个氧原子成键。
Ice-three (Ice III ) - London South Bank University
Ice-three (ice III) is formed from water at 300 MPa by lowering its temperature to 250 K (see Phase Diagram). It is stable over a relatively small range of conditions in the P-T phase space.
The Structure of Ice III - AIP Publishing
The analysis of the ice III diffraction patterns leads to a body‐centered orthorhombic structure, and a unit cell of dimensions a =10.20A, b =5.87A, and c =7.17A. The unit cell contains sixteen …
Water ice phases II, III, and V: Plastic deformation and phase ...
We found ice II to be the strongest of the high-pressure phases, having a strength roughly comparable to that of ice I. Ice III is very weak: at fixed levels of stress, ice III flows 10 2 -10 3 …
Structure of ice III - Acta Crystallographica Section B
Ice III, least dense of the high pressure forms of ice (0c= 1.160 g.cm-3 at -175°C, 1 atm), has a tetra- gonal structure (P41212, a= 6.73, c= 6.83/~,) involving a tetrahedrally linked H-bond …
Transformations of Ice II, Ice III, and Ice V at Atmospheric Pressure
The transformations that occur in ices II, III, and V at atmospheric pressure when they are heated from liquid‐nitrogen temperature have been examined by simple thermal analysis and by x‐ray …
Thermodynamics of high-pressure ice polymorphs: ices III and V
2004年7月1日 · Thermodynamic properties of high-pressure ice polymorphs, ices III and V, are studied theoretically. The results of TIP4P molecular dynamics simulations in the NPT …
Metastable ice-three may be formed within the ice-two phase space by raising the compression rate in the density driven phase transition from hexagonal ice down to 170 K [1545].