非局域密度泛函理论表征活性炭孔径分布的改进算法

为提高由NLDFT计算值确定活性炭孔径分布(PSD)的精度,根据测得的77K氮在非石墨化碳黑BP460和椰壳活性炭K05上的吸附数据,比较了吸附空间及壁面结构采取不同假设对计算结果的影响。结果表明,常规将活性炭吸附空间近似为无限尺寸的石墨化碳黑表面构成的狭缝孔,并由Lorenz-Berthelot混合法则确定相互作用参数,计算值在较低压力区域和试验值之间的偏差明显;而将吸附壁面结构近似为非石墨化碳黑,并由表面粗糙度和石墨晶格分布的误差函数修正相互作用参数后,计算结果和试验值吻合良好。分析结果时发现,归一化方法和考虑周边吸附质分子作用的加权函数是影响NLDFT计算结果准确性的关键因素。     

低温容器内活性炭吸氢性能的模拟研究

以石墨片微元构建活性炭的结构模型,采用巨正则蒙特卡罗(GCMC)方法从微观研究H_2在以活性炭为基的复合吸氢剂中的吸附特性,获得了不同条件下复合吸氢剂对H_2的吸附过程。结果表明,氧化物吸氢剂修饰对活性炭材料的表面化学性能影响较大,引入之后使其吸氢量增加了一倍以上;氧化物吸氢剂嫁接在活性炭上的不同位置吸氢效果不同,以双键连接位置为佳;在低温领域选择PdO的替代材料时,温度为77 K时,优选顺序为Cu_2OAg_2OCuO,当温度为90.5 K、111 K、194.5 K时,优选顺序为CuOCu_2OAg_2O。     

氙(Xe)原子在铂(Pt)表面吸附与脱附的分子动力论方法研究

运用分子动力论方法研究单原子气体分子(Xe)在固壁表面(Pt)的吸附与脱附。在构造了合理的气体分子与固壁表面相互作用势模型之后,运用随机经典轨道方法求解气体分子及固壁原子的运动方程,得到气体分子的运动轨迹及状态。结果表明,气体分子在固壁表面的吸附几率与分子的入射平动能量、壁面温度及气-固相互作用势模型的选取等因素有关,气体分子在固壁表面的脱附速率基本满足Arrhenius关系式。     

乙烷在中孔分子筛MCM-41中吸附的计算机分子模拟

采用计算机模拟方法研究不同温度下乙烷在不同孔径的MCM-41中的吸附.其中乙烷分子采用两个LJ中心的势模型表征，乙烷分子与MCM-41孔壁的相互作用采用一个连续的势模型表示.除考察了温度、孔径对吸附量的影响外，还研究这些量对乙烷分子在孔中的甲基和质心的分布，以及它们对乙烷分子在孔中的排列方向的影响.GCMC模拟结果发现，在180K和300K时壁面处都有较多的乙烷分子倾向于沿着壁面排列，同时在180K时其余的流体分子倾向于垂直于壁面排列，而在300K时其余的分子并不像在180K时一样倾向于垂直于壁面排列.模拟结果还表明，除壁面附近外，即使是在180K的较低温度下，乙烷分子的排列也是混乱和无序的.     

气体临界温度以上吸附平衡的预测研究

采用容积法测定了CH4和N2 在微孔活性炭K0 2上的吸附平衡数据 ,温度为 2 73～ 333K ,压力为 0～12MPa .提出了一个可以从单一气体吸附等温线预测其它条件下吸附平衡的理论模型 .该模型考虑了临界温度以上吸附相密度和饱和吸附量与温度的关系 ,并采用孔径分布来表征吸附剂表面吸附势场的不均一性 ,局部方程使用Langmuir描述 .利用此模型预测了CH4和N2 在K0 2活性炭上的吸附平衡 ,在所研究的温度、压力范围内的整体预测偏差不超过 3% .另外 ,对文献中不同实验条件下气体临界温度以上的吸附平衡进行了研究 ,在较宽的范围内也取得了很好的预测结果     

低温吸附泵用椰壳活性炭的性能测试

活性炭的比表面积、孔径及分布是影响液氦低温吸附泵抽氢、氦性能的关键因素。为了确定制作液氦低温吸附泵的吸附剂,选取了C1、C2、C3、C4四种椰壳活性炭,用比表面积及孔径分析仪测定了其等温吸附性能,并对实验数据进行了针对性分析,获得了各活性炭的比表面积、微孔比表面积份额、不同孔径所对应的孔容等性能数据。结果表明,四种活性炭中C2最适于做为抽氢、氦的液氦低温吸附泵的吸附剂。     

氢气在炭狭缝微孔内吸附的预测

通过边界的平均场近似,推导二平板狭缝孔格子理论Ono-Kondo吸附等温方程。利用格子模型特性和微观物理学理论,计算氢分子在石墨平面的最大吸附容量。比较由氢分子在石墨平面二典型聚集状态标定的Ono-Kondo方程,并用预测精度较高的方程计算了与文献相同条件下的吸附等温线。在比较了计算结果、试验结果和GCMC分子模拟结果后,对Ono-Kondo吸附等温方程的特点、理论基础作了分析,指出了方程的适用范围。     

溴素改性活性炭汞吸附特性研究

在固定床实验台上进行了1%NH_4Br改性活性炭汞吸附实验。利用吸附动力学模型从动力学角度探讨了汞吸附速率控制步,汞吸附活化能与初始汞吸附速率。结果表明:150℃时,1%NH_4Br改性活性炭脱汞能力显著增强,其原因是改性后活性炭表面活性位点(Br)明显增加,强化了化学吸附作用。但低温时,化学吸附增强作用不明显。汞在改性活性炭表面的吸附活化能为29.69 kJ/mol,说明吸附以物理吸附为主,化学吸附为辅。改性活性炭的初始汞吸附速率随温度增加而增加。活性位吸附是汞吸附速率控制步,外部传质控制也影响整个汞吸附过程,吸附遵循Langmuir吸附等温方程。     

载硫椰壳活性炭喷射脱汞实验研究

以元素硫对椰壳活性炭在不同温度下进行载硫改性。采用N2吸附/脱附、X射线近边吸收结构等方法对吸附剂进行孔隙结构和硫存在形态表征。在模拟烟气管道喷射实验装置上进行汞吸附脱除实验研究。载硫温度500℃时椰壳活性炭汞吸附效率优于商用富硫活性炭。活性炭汞吸附脱除能力由孔隙结构、硫含量与存在形态共同决定。不同体积分数SO_2、NO和HCl的加入对活性炭均有不同程度的促进作用。     

吸附氢分子的振动态及熵的计算

用第一性原理方法研究了H_2在(MgO)_9及(AlN)_(12)团簇上的吸附态、振动模式及熵.分析表明,吸附体系的振动中有六个简正模式可归为氢分子的振动;由于氢分子质量很小,零点能修正对吸附能有重要影响.利用振动配分函数计算了吸附氢分子的熵,表明吸附态H_2的熵主要决定于较低的同相振动的频率,并不完全与吸附强度相关;在标准大气压下70—350 K的温度范围内,吸附H_2的熵与气态H_2的熵之间存在很好的线性关系,吸附后H_2的熵减小约10.2R.     

碳纳米纤维吸附储氢性能分析

文中综合碳纳米纤维微观结构的表征结果以及氢吸脱附等温线的实验测量结果,对碳纳米纤维的吸附储氢性能进行了综合分析,分析发现:比表面积和中孔容积均与氢吸附量成线性关系;微孔容积对材料吸附性能影响较大,微孔容积与氢吸附量成抛物线关系;氢在常温左右以及77K下的吸附等温线呈现超临界气体的吸附特征,氢在273K和353K下的吸脱附等温线也基本重合,呈现的是物理吸附的特征。实验结果还说明:常温左右,甚至是77K下,碳纳米纤维均不适合于氢的吸附储存。     

氢在多壁碳纳米管中的吸附储存

利用巨正则系综蒙特卡罗(GCMC)的方法模拟了氢在多壁碳纳米管中的吸附,氢气分子之间、氢气分子和碳原子之间的相互作用势能采用Lennard-Jones势能模型。模拟了不同结构参数(管内径、管壁数、管壁间距)的多壁碳纳米管在77K和298K下的吸附等温线,分析了多壁碳纳米管的管内径、管壁数以及管壁间距对吸附性能的影响。模拟结果表明:多壁碳纳米管的管壁数和管壁间距对吸附性能的影响较明显;管壁数越少,管壁间距越大,其吸附性能越好;多壁碳纳米管的管内径对其吸附性能的影响甚微。     

Molecular dynamics simulations of hydrogen adsorption/desorption by palladium decorated single-walled carbon nanotube bundle

Utilising molecular dynamics simulations, the hydrogen molecules adsorption isotherms of the (8,?0) palladium decorated single-walled carbon nanotube (SWNT) were obtained. The hydrogen adsorption was studied on the external, interstial and internal surfaces of the SWNT bundle at several temperatures ranging from 77 to 400?K. The results were compared with the bare single-walled carbon nanotube bundle under the same conditions. The decorated carbon nanotube bundle hydrogen adsorption was significantly higher than that of the bare one. The hydrogen desorption and readsorption were studied using temperature as the readsorption/desorption variable. The rate constants were calculated for the hydrogen desorption at different temperatures. The calculated decorated SWNT bundle hydrogen desorption activation energy was higher than that for the bare SWNT bundle. The calculated activation energies for the hydrogen desorption in both nanotube bundles specified the temperature dependency of hydrogen desorption.     

CO2 adsorption and reaction on Fe(111): An angle resolved photoemission (ARUPS) study

Molecular CO₂ adsorption is observed on an Fe(111) surface at 85 K. For the main fraction of molecules the relative binding energies of the valence ion states as determined by ARUPS are consistent with those in the gas as well as in the condensed phase, and indicate that the electronic structure of that fraction of adsorbed molecules is only slightly distorted upon adsorption. There is a fraction of adsorbed molecules at 85 K that can be identified as bent, anionic CO₂⁻ species. While the weakly adsorbed, linear CO₂ molecules desorb at low temperature, the CO₂⁻ species is stable up to 160–180 K. The latter is proposed to be a precursor to dissociation. Above this temperature adsorbed carbon monoxide and oxygen are observed on the surface, and at room temperature the CO₂⁻ signals have disappeared. Heating above room temperature dissociates the CO molecules into carbon and oxygen.     

Interaction between nanobuds and hydrogen molecules: A first-principles study

Hydrogen storage materials are crucial for the wide application of hydrogen in fuel cells. In this Letter, the interaction between hydrogen molecules and nanobuds has been studied using the Dmol3 package. The results show that the adsorption energies of hydrogen molecules onto nanobuds range from 0.069 eV to 0.115 eV, and that the adsorption energies are not sensitive to the nanobuds' structures but closely related to the number of carbon atoms around H₂ molecules. The energy barrier of a hydrogen molecule entering C176 is 2.38 eV. Each C176 nanobud can accommodate four H₂ molecules. The stress existing in nanobuds induces alterative charge distribution, which can improve the hydrogen storage performance of nanobuds to a certain extent.     

The chiral effect of adsorption of univalent atoms and diatomic molecules on the surface of carbon nanotubes

Quantum-chemical semiempirical calculations were performed of the adsorption of fluorine and hydrogen atoms and molecules on the surface of single-layered carbon nanotubes with various diameters. Semiempirical quantum-chemical MNDO calculations were based on the model of a molecular cluster with boundary pseudoatoms. The energy characteristics of adsorption were determined. Changes in physical properties caused by the adsorption of atoms and diatomic molecules were analyzed.     

Coverage dependence of neopentane trapping dynamics on Pt(111)

Adsorption probabilities for neopentane on Pt(111) were measured directly using supersonic molecular-beam techniques at coverages ranging from zero to monolayer saturation, incident translational energies between 18 and 110 kJ mol⁻¹ and incident angles between 0° and 60° at a surface temperature of 105 K. The adsorption probability was found to increase with coverage up to near monolayer saturation at all incident translational energies and incident angles. The coverage dependence of the adsorption probability predicted by a modified Kisliuk model with enhanced trapping into the second layer exhibits good quantitative agreement with the experimental values. The angular dependence of the adsorption probability decreases with increasing coverage, suggesting that the effective corrugation of the gas–surface interaction potential increases with the adsorbate coverage. The initial adsorption probability into the second layer onto the covered surface decreases from 0.95 to 0.75 with increasing energy over the energy range studied, and exhibits total energy scaling. A comparison with second-layer trapping data of simpler molecules onto covered Pt(111) indicates that the structural complexity of adsorbed neopentane molecules facilitates collisional energy transfer during adsorption.     

硫在Fe(100)面吸附的第一性原理研究

基于密度泛函理论的第一性原理方法,在广义梯度近似下,计算了硫原子在Fe(100)面吸附的结构和电子性质,并计算了其分子轨道和吸附能.同时讨论了相关吸附性质与硫原子表面覆盖度(0.25-1.0ML)的关系.结果表明：硫原子吸附在H位最稳定,吸附能均随浓度的增加而单调增加;B位吸附的硫原子与Fe(100)表面的距离随浓度非单调变化,在0.5ML时达到最大,是由较高的局域电子云重叠产生的排斥作用所导致的;对比分析吸附前后硫和Fe的s及p电子的态密度,显示了硫化亚铁的生成.     

Kinetics of the decomposition of disilane molecules on a silicon growth surface in vacuum chemical epitaxy

In the framework of the kinetic approach based on data of technological experiments, the range of characteristic rates of decomposition of disilane radical molecules adsorbed on the surface during the growth of a silicon layer is determined. The relationship between the rate of incorporation of silicon atoms into a growing crystal and the characteristic rate of pyrolysis of hydride molecules on the growing surface is established. The temperature dependences of the decomposition rate of disilane molecules exhibit an unusual activationless behavior in the growth temperature range. The form of the observed dependences is determined by the pyrolysis model, conditions of transferred of hydrogen from an adsorbed molecule onto the surface of the growing layer, being a function of the gas pressure and temperature in the reactor. It is demonstrated that the basic features of the behavior of the decomposition rate of disilane molecules are controlled by the specifics of the interaction of the silicon dihydride molecular beam with the growth surface under conditions of low and high degrees of bonding of hydrogen to free surface bonds. The temperature dependences are qualitatively described by a relation composed of two activation curves with different activation energies at low and high temperatures and preexponential factors depending on the surface coverage by hydrogen atoms.