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Self-diffusion of supercritical water in extremely low-density region

机译:超临界水在极低密度区域的自扩散

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The self-diffusion coefficient D for super- and subcritical water is determined by using the proton pulsed-field-gradient spin echo method at high temperatures and low densities. The density of water is ranged in the steamlike region from 0.0046 to 0.0650 g cm(-3) at a supercritical temperature of 400 degrees C, also at 0.0046-0.0079 and 0.0046-0.0462 g cm(-3) (the steam-branch densities on the coexistence curve and lower) at 200 and 300 degrees C, respectively. The density is precisely determined on the basis of the PVT dependence of the proton chemical shift. The density-diffusivity products in the zero-density limit divided by the square root of the temperature, (rho D)(0)/root T, are 1.03, 1.28, and 1.44 fg m(-1) s(-1) K-1/2 (f, femto) at 200, 300, and 400 degrees C, respectively. The (rho D)(0)/root T obtained decreases with decreasing temperature and is significantly smaller than the temperature-independent value from the hard sphere model, 1.95 fg m(-1) s(-1) K-1/2. The marked temperature dependence reflects the presence of the strong attractive interaction between a pair of water molecules. The magnitude of the experimental D values and the temperature dependence are well reproduced by the molecular dynamics simulation using TIP4P-FQ model. The initial slope of the product rho D/root T against rho is almost zero at 400 degrees C and slightly negative at 300 degrees C. (c) 2006 American Institute of Physics.
机译:通过在高温和低密度下使用质子脉冲场梯度自旋回波方法来确定超临界和亚临界水的自扩散系数D。在400摄氏度的超临界温度下,水样区域的蒸汽密度范围为0.0046至0.0650 g cm(-3),也为0.0046-0.0079和0.0046-0.0462 g cm(-3)(蒸汽分支密度)分别位于200和300摄氏度时。密度是基于质子化学位移的PVT依赖关系精确确定的。零密度极限中的密度-扩散乘积除以温度的平方根(rho D)(0)/根T为1.03、1.28和1.44 fg m(-1)s(-1)K -1/2(f,femto)分别在200、300和400摄氏度下发生。 (r D)(0)/根T随温度降低而降低,并且显着小于硬球模型的温度无关值1.95 fg m(-1)s(-1)K-1 / 2。明显的温度依赖性反映了一对水分子之间存在强吸引力的相互作用。通过使用TIP4P-FQ模型进行的分子动力学模拟,可以很好地再现实验D值的大小和温度依赖性。产物rho D /根T相对于rho的初始斜率在400摄氏度时几乎为零,在300摄氏度时略为负。(c)2006美国物理研究所。

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