2005
DOI: 10.1107/s0021889805014226
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The incompressibility and thermal expansivity of D2O ice II determined by powder neutron diffraction

Abstract: Using high-resolution neutron powder diffraction, the molar volume of a pure sample of D 2 O ice II has been measured, within its stability field, at 225 K, over the pressure range 0.25 < P < 0.45 GPa. Ar gas was used as the pressure medium, to avoid the formation of 'stuffed ice' gas hydrates encountered when using He.

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Cited by 47 publications
(65 citation statements)
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“…3 The circles and the solid line drawn through them show the experimental results for heavy ice II at -48°C fitted with a Birch-Murnaghan equation. 15 from -78 to -12°C. In particular, the difference in the compressibilities of "pure" and He-filled ice II is below the error level.…”
Section: Resultsmentioning
confidence: 99%
“…3 The circles and the solid line drawn through them show the experimental results for heavy ice II at -48°C fitted with a Birch-Murnaghan equation. 15 from -78 to -12°C. In particular, the difference in the compressibilities of "pure" and He-filled ice II is below the error level.…”
Section: Resultsmentioning
confidence: 99%
“…38,39 It forms upon compression of ice Ih below 238 K at ∼0.2 GPa, and its region of thermodynamic stability is separated from the liquid phase by other high-pressure phases. 40,41 Ice II is a fully hydrogen-ordered form of ice with R3 space group symmetry.…”
Section: A Background: Ices Ih II V and Xiiimentioning
confidence: 99%
“…The comparison of the QHA result to available experimental data 21,64 at atmospheric pressure is presented in Fig. 5 for deuterated ices Ih and II.…”
Section: A Thermal Expansionmentioning
confidence: 99%
“…The experimental results for D 2 O ice at 145 K (ice Ih) 66 and 225 K (ice II) 64 are compared to the QHA expectation in Fig. 7.…”
Section: Gpamentioning
confidence: 99%