AbstractThe saturation loadings for subcritical adsorption of multi-atomic inorganic species, halocarbons and ox'/> Saturation loadings on 13X (Faujasite) zeolite above and below the critical conditions. Part?IV: inorganic multi-atomic species, halocarbons and oxygenated hydrocarbons data evaluation and modeling
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Saturation loadings on 13X (Faujasite) zeolite above and below the critical conditions. Part?IV: inorganic multi-atomic species, halocarbons and oxygenated hydrocarbons data evaluation and modeling

机译:在临界条件上方和低于临界条件的13x(faujasite)沸石上的饱和载荷。 部分?IV:无机多原子物种,卤素和含氧烃数据评估和建模

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AbstractThe saturation loadings for subcritical adsorption of multi-atomic inorganic species, halocarbons and oxygenated hydrocarbons on 13X zeolite are modeled using the modified Rackett model of Spencer and Danner (J. Chem. Eng. Data 17(2):236–240, 1972) for the saturated liquid densities combined with crystallographic data for the 13X zeolite. A similar equation is used for supercritical adsorption involving supercritical adsorbate densities and crystallographic data for the 13X zeolite employing a differentf(Tr) expression than used by Spencer and Danner. Adsorption data from the literature are first critically evaluated and then compared to the model. Log–log plots are used to determine whether each isotherm is near saturation; isotherms that exhibit a$$left( {partial ln q} ight)/left( {partial ln p} ight)$$?lnq/?lnpslope of zero at the maximum pressure point are assumed to be saturated (capillary condensation points are deleted). The highest loading is used from each isotherm that approaches saturation. Unsaturated isotherms are not considered further. The theoretical equation satisfactorily models the available experimental data for the data that is subcritical except for water and methanol. However, steric factors are required in the model for tetrafluoromethane, sulfur hexafluoride and the aldehydes. The adsorption data for ethyl acetate is questionable. A significant amount of data in the supercritical region (tetrafluouromethane, and hexafluoroethane) revealed a decreasing trend with increasing Tr. For this data af(Tr) is modeled using TCARand the slope of the decreasing linear plot against Tr. The physical phenomenom causing this effect is attributed to increasing molecular vibration in the cavity reducing the total molecular loading with temperature rise.]]>
机译: F (T <下标> R )表达式的13x沸石的晶体学数据而不是使用斯宾塞和丹纳。从文献中的吸附数据首先受到批判性评估,然后与模型进行比较。日志日志图用于确定每个等温器是否接近饱和度;表现出 $$ left({ partial ln q} left)/ left({ partial ln p} revents)$$ ln q / ln p < / mfeced> 在最大压力点处的零点被认为是饱和的(毛细血管冷凝点被删除)。从每个等温线使用的最高载荷饱和。不饱和等温线未进一步考虑。理论方程令人满意y模拟除水和甲醇外的数据的可用实验数据。然而,在四氟甲烷,六氟化硫和醛的模型中需要空间因子。乙酸乙酯的吸附数据是可疑的。超临界区(四氟甲烷和六氟乙烷)中的大量数据显示出降低趋势,随着T <下标> R 增加。对于该数据,使用T <下标> CAR 和缩小线性图的斜率来建模<重点类型=“斜体”>(t <下标> R )。 <下标> R 。导致这种效果的物理现象归因于腔内的分子振动,降低了温度升高的总分子负荷。 ]]>

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