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Henry's law behavior and density functional theory analysis of adsorption equilibrium.

机译:亨利定律行为和密度泛函理论分析吸附平衡。

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This work focuses on three different aspects of adsorption equilibrium: the measurement of adsorption equilibrium into the Henry's law region for n-pentane, the calculation of the maximum isosteric heat of adsorption achievable in the Henry's law region for slit-shaped pores, and the incorporation into density functional theory of statistical associating fluid theory to treat the adsorption of chain molecules in slit-shaped pores and analyze data for nitrogen and pentane adsorbed in activated carbon.;In the first section experimental data for n-pentane adsorbed on BPL activated carbon in a nitrogen environment are reported at ultra-low concentrations into the Henry's law region. We introduce two methods to prepare pre-equilibrated samples at known loadings. The samples were analyzed by a purge and trap method. Adsorption data were measured at loadings from 1.0 down to 0.0001 mol kg -1 and pressures of 6 down to 5 x 10-10 kPa. The transition into the Henry's law region occurs over a range of loadings near 0.01 mol kg-1 for all temperatures. The data are compared with the DR, Langmuir, and Toth equations. We discuss how the three equations transition into the Henry's law region, and how well they describe the data. Since the DR equation does not have a proper Henry's law region, we show where this equation no longer applies. The Toth equation describes the data better than the Langmuir equation.;The second section discusses the isosteric heat of adsorption in the Henry's law region calculated as a function of the width of slit-shaped pores. We determine the pore width where the isosteric heat is a maximum, which is shown to be a strong function of the solid-fluid collision diameter sigma sf and a weak function of the solid-fluid well depth potential epsilon sf. Thus, general results are reported for the pore size where the isosteric heat of adsorption is a maximum that apply to a wide variety of gases. We compare our values of isosteric heat with those in the Henry's law region determined from adsorption data for nitrogen, argon, carbon dioxide, and methane on various activated carbons. The isosteric heats of adsorption for helium and hydrogen in carbon slit pores are also calculated, but are not compared with experimental data. Reasons for differences between the theoretical maximum and the experimental values are discussed.;In the third section density functional theory is modified to include the statistical associating fluid theory equation of state in order to describe chain fluids. First-order non-mean field and second-order perturbation attractive terms are included in the model. The interaction parameters for both nitrogen and n-pentane with a carbon parallel slit pore are determined. The monolayer transition, pore condensation, and a clear freezing transition are observed for nitrogen. The effects of the pore size on when the transitions occur is discussed. The pore size distribution for BPL activated carbon is calculated from an experimental nitrogen isotherm and the model. The monolayer transition and pore condensation for n-pentane are found. An isotherm for n-pentane is calculated using the nitrogen pore size distribution and the n-pentane model.
机译:这项工作着眼于吸附平衡的三个不同方面:正戊烷在亨利定律区域的吸附平衡的测量,狭缝形孔在亨利定律区域可达到的最大吸附等规吸附热的计算以及结合引入统计缔合流体理论的密度泛函理论来处理狭缝状孔中链分子的吸附,并分析活性炭中吸附的氮和戊烷的数据。据报道,进入亨利定律地区的氮环境浓度超低。我们介绍了两种在已知载荷下制备预平衡样品的方法。通过吹扫捕集法分析样品。在1.0至0.0001 mol kg -1的负载量和6至5 x 10-10 kPa的压力下测量吸附数据。在所有温度下,都在接近0.01 mol kg-1的一系列载荷范围内发生了向亨利定律区域的过渡。将数据与DR,Langmuir和Toth方程进行比较。我们讨论了这三个方程如何过渡到亨利定律区域,以及它们如何很好地描述数据。由于DR方程没有适当的亨利定律区域,因此我们说明该方程不再适用的地方。 Toth方程比Langmuir方程更好地描述了数据。第二部分讨论了亨利定律区域中的吸附等规热,它是狭缝形孔的宽度的函数。我们确定等排热最大的孔径,这是固液碰撞直径σsf的强函数,而固液阱深度势εsf的弱函数。因此,据报导了孔径的一般结果,其中等规吸附热是最大的,适用于各种气体。我们将等排热值与亨利定律中的值进行比较,该值由各种活性炭上的氮,氩,二氧化碳和甲烷的吸附数据确定。还计算了碳缝隙孔中氦和氢的吸附等排热,但未与实验数据进行比较。讨论了理论最大值与实验值之间差异的原因。第三部分,对密度泛函理论进行了修改,使其包括统计缔合流体理论的状态方程,以描述链流体。一阶非均值场和二阶摄动吸引项包含在模型中。确定了氮和正戊烷与碳平行狭缝孔的相互作用参数。对于氮,观察到单层转变,孔凝结和清晰的冷冻转变。讨论了孔径对过渡时间的影响。 BPL活性炭的孔径分布是根据实验氮等温线和​​模型计算得出的。发现了正戊烷的单层过渡和孔缩合。使用氮孔径分布和正戊烷模型计算正戊烷的等温线。

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