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首页> 外文期刊>Journal of Chemical and Engineering Data: the ACS Journal for Data >Density, Viscosity, Speed of Sound, Bulk Modulus, Surface Tension, and Flash Point of Binary Mixtures of n-Hexylbenzene (1) or n-Butylbenzene (1) in 2,2,4,6,6-Pentamethylheptane (2) or 2,2,4,4,6,8,8-Heptamethylnonane (2) at 0.1 MPa
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Density, Viscosity, Speed of Sound, Bulk Modulus, Surface Tension, and Flash Point of Binary Mixtures of n-Hexylbenzene (1) or n-Butylbenzene (1) in 2,2,4,6,6-Pentamethylheptane (2) or 2,2,4,4,6,8,8-Heptamethylnonane (2) at 0.1 MPa

机译:在2,2,4,6,6-五丁醇甲烷(2)中的正己苯(1)或正丁基苯(1)中的二元混合物的密度,粘度,声音,表面张力和闪点闪点(1) 2,2,4,4,6,8,8-8-庚烷(2)在0.1MPa下

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This work reports physical property measurements of binary mixtures of n-hexylbenzene (1) and n-butylbenzene (1) in 2,2,4,6,6-pentamethylheptane (2) and 2,2,4,4,6,8,8-heptamethylnonane (2) at temperatures within the range 253.15-333.15 K. Mixture densities, speeds of sound, and calculated bulk moduli increased with increasing aromatic compound concentration. Excess molar volumes were positive for 2,2,4,4,6,8,8-heptamethylnonane mixtures, negative for hexylbenzene/2,2,4,6,6-pentamethylheptane mixtures, and close to zero for butylbenzene/2,2,4,6,6-pentamethylheptane mixtures at 293.15 K. Excess speeds of sound were positive for all mixtures at 298.15 K, except for n-butylbenzene/,2,2,4,4,6,8,8-heptamethylnonane mixtures, which were close to zero. These results show that compressibility as well as volume change is important for excess speeds of sound. Kinematic viscosities decreased as the aromatic concentration increased at 293.15 K, except for hexylbenzene (x(1)) in 2,2,4,6,6-pentamethylheptane, where increasing hexylbenzene caused a slight viscosity decline before increasing to the value for hexylbenzene. Viscosities were successfully modeled using the McAllister equation. The excess molar Gibbs energy of activation for viscous flow at 293.15 K was not statistically different from zero, which suggests ideal behavior for viscosity. Mixture surface tensions at room temperature and flash points fell within the values of the pure components. Many of these mixtures have property values similar to those of petroleum-based diesel and jet fuel.
机译:该工作报告了二己基苯(1)和正丁基苯(1)中的二元混合物的物理性质测量在2,2,4,6,6-五丁基甲基甲烷(2)中,2,2,4,4,6,8在253.15-333.15k的温度下,8-庚烷(2)在253.15-333.15k的温度范围内。混合密度,声速和计算的本体模量随着芳族化合物浓度的增加而增加。对于2,2,4,4,6,8,8-庚烷混合物的多余摩尔体积是阳性的,对于己苯/ 2,2,4,6,6-五甲基庚烷混合物负,并且对于丁基苯/ 2,2℃下接近零。 ,4,6,6-五甲基庚烷混合物在293.15k。除了正丁基苯/,2,2,4,4,6,8,8-己酰基甲基混合物外,除了正丁基苯/,2,2,4,4,6,8,8-庚烷混合物之外,所有混合物的声音过多为298.15k的阳性。这接近零。这些结果表明,压缩性以及体积变化对于过度的声音很重要。除了2,2,4,6,6-五丁基甲烷中的己苯(x(1))外,芳香浓度在293.15k中增加时,运动粘度降低,其中在增加己烯苯导致己烯苯的值之前导致轻微的粘度下降。使用McAllister方程成功建模了粘度。 293.15K在293.15k的粘性流动激活的过量磨牙能量与零统计学不同,这表明粘度的理想行为。室温下的混合物表面张力和闪点下降在纯组分的值内。这些混合物中的许多具有与石油基柴油和喷射燃料类似的性质值。

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