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1.
金属钯表面吸附氢同位素的量子力学计算   总被引:2,自引:0,他引:2  
基于原子分子反应静力学和群论,应用密度泛函方法B3P86,对H(D,T)用基集合6311G,对Pd用基集合SDD,优化后进行势能面扫描,得到各分子的微观性质,包括构形、多重性、能量、电子状态、键角、平衡键长、谐振频率、谐性力常数和离解能,得到H2(D2,T2)和PdH(PdD,PdT)的电子状态分别为1Σ+g(D∞v)和2Σ+(C∞v),离解能分别为4.5918和2.6268eV.并进一步计算得到反应过程的△Hf°、△Sf°、△Gf°和平衡压力,并导出他们与温度的函数关系,计算结果与实验数据相近.  相似文献   

2.
金属镍吸附氢同位素的量子力学计算   总被引:18,自引:8,他引:10  
根据原子分子反应静力学与群论,确定了NiH、NiD和NiT的基电子状态为2Σ+。应用基函数6-311G和组态相关CI或QCISD方法,计算了氢同位素分子及其镍化物的能量E、定容热容Cv和熵S。设用总能量中的电子和振动能量近似代表NiH、NiD和NiT分子处于固态时的能量,用总熵中的电子和振动熵近似代表这些分子处于固态时的熵,进而计算了镍吸附H2、D2和T2分子过程的ΔH°、ΔS°、ΔG°和平衡压力,并导出它们与温度的函数关系。计算指出了同位素分子效应,结果合理。所以,本文所建议的用量子力学方法计算多相化学反应,有应用参考价值。  相似文献   

3.
用原子分子反应静力学与群论的方法,推导了AlH、AlD及AlT的基电子状态为1Σ+。在QCISD/6-311G水平上对氢化铝进行了计算,导出了其MurrelSorbie势能函数,并计算了氢同位素分子及其铝化物的能量E和熵S。设用总能量中的电子和振动能量近似代表AlH、AlD和AlT分子处于固态时的能量,用总熵中的电子和振动熵近似代表这些分子处于固态时的熵,进而计算了铝吸附H2,D2和T2分子过程的ΔH°,ΔS°,ΔG°和平衡压力,并导出它们与温度的函数关系,计算指出了同位素分子效应,结果合理。  相似文献   

4.
氢同位素双原子分子的解析势能函数   总被引:17,自引:0,他引:17  
研究从重水中分离出T2 .首先 ,根据光谱常数导出氢同位素双原子分子ExtendedRydberg的分析函数 ,基于同位素效应计算OT(X2 Пi)的光谱常数 ,有助导出三原子分子 ,如DTO的解析势能函数 .将这些ExtendedRyd berg解析势能函数用于氘交换分离氚的热力学与分子反应动力学研究 .此外 ,由同位素位移极值得到当振动量子数vmax≈ 11.5 ,振动能级间隔△Ev(H2 )≈△Ev(T2 ) ,若v △Ev(T2 )和v>vmax时 ,△Ev(H2 ) <△Ev(T2 ) .因而 ,温度较低时 ,平衡移向T2 ;温度较高时 ,平衡移向H2 .与文献结果相似 ,而导出方法不同  相似文献   

5.
金属Pt表面氢同位素解离吸附的热力学研究   总被引:1,自引:0,他引:1  
基于电子与振动近似方法和密度泛函B3LYP理论,对氢原子采用6-311G"基函数,Pt选择赝势基组LanL2DZ,优化得到Pt-H和Pt-H2结构和微观性质,Pt-H分子平衡键长和谐振频率分别为0.1528nm和2336cm-1,与实验值一致.氢气分子吸附于Pt表面反应的Gibbs自由能⊿G0为正值,远大于解离反应⊿G0值,氢气在Pt表面不能以完整分子形式与Pt结合,易于解离成氢原子.计算了氢同位素在Pt表面解离反应的⊿S0,⊿H0,⊿G0和平衡压力,并导出它们与温度的关系.由⊿G=0kJ.mol-1计算得0.1MPa时H2,D2和T2的脱附温度分别为962K,919K和892K,大多数反应Pt-H(D或T)都能稳定存在.  相似文献   

6.
7.
在Pu的相对论有效原子实势近似和O原子6-311G*全电子基函数下,用quadratic configuration interaction of singlely and doublely substitution(QCISD)方法计算了PuO分子基态X5Σ-的Murrell-Sorbie解析势能函数和热力学函数,得到Re,De,Bee关键词:  相似文献   

8.
计算氢同位素水分子汽化焓的比较法   总被引:2,自引:0,他引:2  
本文首次提出计算氢同位素水分子汽化焓的比较法,得到0~374℃时H2O,D2O,DTO和T2O的汽化焓,并提出用D2从含氚重水中分离出DT气的适宜温度.  相似文献   

9.
黄刚  龙兴贵  彭述明 《光谱实验室》2010,27(5):2037-2041
激光拉曼光谱作为一种非侵入式的物质结构和成分分析的测试手段特别适合于核工业中含氚放射性同位素气体的定性和定量分析。将经典物理学方法和量子力学理论相结合,采用非刚性转子校正模型,计算获得了H2、HD、HT、D2、DT、T26种氢同位素气体分子的转动跃迁拉曼频移,为氢同位素气体拉曼光谱谱峰的辨识提供理论数据。通过实验测定H2和D2的转动拉曼光谱,得到这2种分子的转动拉曼图谱和拉曼频移,并将测定结果与计算结果进行比较,验证了理论计算方法的可行性和正确性。  相似文献   

10.
本文讨论了气固多相反应的一般条件,同时,根据文献[1]的H2-Ni系统的平衡压力,进一步计算H2在Ni(β)中的溶解度为338.11~966.55(cm3)/(cm3atm 1/2),溶解热为-4 064.06~-4 316.24 cal以及溶解度系数公式为S=T 0.464 8exp(4 894.33)/(RT),均与文献相合.这也表明文献[1]所建议的电子振动近似法的正确性.  相似文献   

11.
119Sn NMR showed that β-tin areas that formed upon freezing at magnetic field 9.4 T on the surface of tin polycrystalline samples have their symmetry axes strongly aligned along a particular direction. The fraction of the oriented frozen tin was found to approach the total amount of the Sn melt on the sample surface.  相似文献   

12.
We perform molecular dynamics simulations of screening by electrons in low energy nuclear reactions, especially between hydrogen isotopes. Quantum effects that corresponds to the Pauli and Heisenberg principle are enforced by constraints. We show that the enhancement of the average cross-section and of its variance is due to the perturbations induced by the electrons. This gives a correlation between the maximum amplitudes of the inter-nuclear oscillational motion and the enhancement factor. It suggests that the chaotic behaviour of the electronic motion affects the magnitude of the enhancement factor.  相似文献   

13.
The adsorption behavior of hydrogen and oxygen on the stepped Ni(311) surface has been investigated by HREELS. A series of metastable phases was found for hydrogen adsorption at low temperatures with a succession of different adsorption sites indicated by the following loss peaks: 55 and 149 meV for the threefold site, shifting with higher coverage to 65 and 155 meV, respectively; 40 and 90 meV for the fourfold site, shifting to 35 and 85 meV with coverage; and 110 and 124 meV for an additional site between close packed rows. Room temperature adsorption of hydrogen leads to the reconstruction of the surface with occupation of three- and fourfold sites, represented by loss peaks at 60 and 145 meV for the threefold site and 74 meV for the fourfold site. This phase is the thermodynamically stable one. Oxygen is most likely initially adsorbed on a bridge site (loss peak at 66 meV). The stepped surface is already oxidized at very low exposures to oxygen, as seen by the characteristic vibration for oxide islands at 55 meV and later by the Fuchs-Kliewer mode of NiO at 68 meV.  相似文献   

14.
Ultra accelerated quantum chemical molecular dynamics method (UA-QCMD) was used to study the dynamics of the hydrogen spillover process on Pt/CeO2 catalyst surface for the first time. The direct observation of dissociative adsorption of hydrogen on Pt/CeO2 catalyst surface as well as the diffusion of dissociative hydrogen from the Pt/CeO2 catalyst surface was simulated. The diffusion of the hydrogen atom in the gas phase explains the high reactivity observed in the hydrogen spillover process. Chemical changes, change of adsorption states and structural changes were investigated. It was observed that parallel adsorption of hydrogen facilitates the dissociative adsorption leading to hydrogen desorption. Impact with perpendicular adsorption of hydrogen causes the molecular adsorption on the surface, which decelerates the hydrogen spillover. The present study also indicates that the CeO2 support has strong interaction with Pt catalyst, which may cause an increase in Pt activity as well as enhancement of the metal catalyst dispersions and hence increasing the rate of hydrogen spillover reaction.  相似文献   

15.
在CVD沉积SiC过程中,载气体H2与沉积SiC基体表面的反应影响沉积速率和沉积产物品质,因此研究这些微观反应机理具有十分重要的科学意义和工程价值。本文基于第一性原理研究了H2在3C-SiC(111)(硅原子暴露面)和3C-SiC(-1-1-1)(碳原子暴露面)面的吸附位置、吸附能、电子结构和覆盖率等吸附情况。发现H2倾向于吸附在3C-SiC(111)面,H原子的最稳定吸附位为OT位(顶位)且属于化学吸附。H2在吸附时会自发解离为两个H原子,以双顶位形式吸附在两个相邻的Si原子上。该过程中基体表面Si原子的电子向H偏移,此时两者的主要相互作用源于Si原子的p轨道和H的s轨道的重叠杂化。通过计算氢气在表面的覆盖率,发现吸附能随着覆盖率的增大而增大,在低H覆盖率(θH≤4/9 ML)下,H原子之间存在着较强的吸引力,随着H覆盖率的增加(θH>4/9 ML),H原子之间排斥力逐渐增大,吸附能增加趋缓,整体结构更加稳定。  相似文献   

16.
A. Nojima 《Surface science》2007,601(14):3003-3011
We have used density functional theory to investigate hydrogen adsorption and diffusion on a W(1 1 0) surface. Hydrogen adsorption structures were examined from low coverage to one monolayer, and a threefold hollow site was found to be the most stable site at all coverages. In contrast to previous assertions, the work function decrease is not due to electron transfer from the hydrogen atoms to the W surface, but due to electron depletion at the vacuum region above the hydrogen atoms. Hydrogen atoms can diffuse via short-bridge sites and long-bridge sites at a coverage of θ = 1.0. Although the calculated activation energy for hydrogen diffusion via a short-bridge site is as small as 0.05 eV, field emission microscope experiments have shown that the activation energy for hydrogen diffusion is about 0.20 eV, which agrees fairly well with our calculated value of the activation energy via a long-bridge site. This discrepancy can be related to hydrogen delocalization on the W(1 1 0) surface, which has been suggested by electron energy loss spectroscopy experiments.  相似文献   

17.
Development of metal borohydrides for hydrogen storage   总被引:1,自引:0,他引:1  
A metal borohydride M(BH4)n is a potential candidate for hydrogen storage materials because of its high gravimetric hydrogen density. The important research issues for M(BH4)n are to control the thermodynamic stability and to achieve the faster reaction kinetics. To clarify the thermodynamic stability, M(BH4)n (M=Mg, Ca∼Mn, Zn, Al, Y, Zr and Hf; n=2-4) were synthesized by mechanical milling and its thermal desorption properties were investigated. The hydrogen desorption temperature Td of M(BH4)n decreases with increasing Pauling's electronegativities χP of M. Because Mn, Zn, and Al borohydrides (χP?1.5) desorb borane, they are too unstable for hydrogen storage applications. The enthalpy changes of desorption reaction ΔHdes can be estimated by using our predicted heat of formation of M(BH4)n ΔHboro and reported data for decomposed products ΔHprod, which are useful indicators for searching M(BH4)n with appropriate stability for hydrogen storage material. In the latter case, microwave processing was adopted for achieving fast reaction kinetics. Among metal borohydrides, LiBH4 was rapidly heated above 380 K by microwave irradiation, 13.7 mass% of hydrogen was desorbed by microwave irradiation. The composites of LiBH4 with B or C desorbed hydrogen within 3 min. Microwave heating aids in realizing faster kinetics of the hydrogen desorption reaction.  相似文献   

18.
姜平国  汪正兵  闫永播 《物理学报》2017,66(8):86801-086801
采用基于密度泛函理论的第一性原理平面波超软赝势方法,在广义梯度近似下,研究了立方WO_3,WO_3(001)表面结构及其氢吸附机理.计算结果表明立方晶体WO_3理论带隙宽度为0.587 eV.WO_3(001)表面有WO终止(001)表面和O终止(001)表面两种结构,表面结构优化后W—O键长和W—O—W键角改变,从而实现表面弛豫;WO终止(001)表面和O终止(001)表面分别呈现n型半导体特征和p型半导体特征.分别计算了H原子吸附在WO终止(001)表面和O终止(001)表面的H—O_(2c)—H,H—O_(2c)…H—O_(2c),H—O_(1c)—H和H—O_(1c)…H—O_(1c)四种吸附构型,其中H—O_(1c)—H吸附构型的吸附能最小,H—O键最短,H失去电子数最多,分别为-3.684 eV,0.0968 nm和0.55e,此吸附构型最稳定.分析其吸附前后的态密度,带隙从吸附前的0.624 eV增加到1.004 eV,价带宽度基本不变.H的1s轨道电子与O的2p,2s轨道电子相互作用,在-8和-20 eV附近各形成了一个较强的孤立电子峰,两个H原子分别与一个O_(1c)原子形成化学键,最终吸附反应生成了一个H_2O分子,同时产生了一个表面氧空位.  相似文献   

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