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1.
锆氢化反应热力学函数的计算   总被引:21,自引:0,他引:21  
用B3LYP/SDD密度泛函方法计算了ZrH的微观性质,气态ZrH(D,T)的能量(E),熵(S)以及 Zr与氢同位素气体反应的热力学函数.在ZrH(s)、ZrD(s)和ZrT(s)的E和S的计算中,近似以分 子总能量中的振动能Ev代替固态能量,以电子和振动熵SEv代替固态熵.在这种近似下,计算了 不同温度下Zr与H2、D2、T2反应的ΔH、ΔG、ΔS及氢化反应平衡压力,导出了与温度 的依赖关系.计算结果表明,ZrH(s)的生成热为161.34 kJ穖ol-1,与实验值(173.5 kJ穖ol -1)接近,表明这种近似处理方法是合理的,可以用于研究贮氢材料氢化反应的热力学.  相似文献   

2.
N2在Pd金属表面的吸附行为   总被引:4,自引:0,他引:4  
对Pd原子采用相对论有效原子实势(RECP/SDD), N原子采用AUG-cc-pVTZ基函数, 利用B3LYP方法计算了PdN和PdN2分子的微观结构以及不同温度下的热力学函数. 以气态分子总能量中的振动能EV代替该分子处于固态时的振动能量, 以电子运动和振动运动熵SEV代替分子处于固态的熵的近似方法, 计算了不同温度下金属Pd与N2反应的ΔHӨ、ΔSӨ、ΔGӨ及氮化反应平衡压力, 导出了氮化反应平衡压力与温度的关系. 由此可看出, 在常压及298.15~998.15 K温度条件下, N2在金属Pd表面的吸附过程以Pd(s) + N2 = PdN2(s)反应进行. 计算得出在标准条件下, PdN(s)的生成焓为254.37 kJ·mol-1, PdN2(s)的生成焓为-80.59 kJ·mol-1. 并与Pd氢化反应平衡压力比较, 得到平衡常数Kp(N2)比Kp(H2)约小两个数量级, 说明N2较难被金属Pd表面吸附, 在热力学上有利于氢置换氮.  相似文献   

3.
用B3LYP/SDD密度泛函方法计算了CoH的微观性质、CoH(g)、CoD(g)和CoT(g)的能量(E)和熵(S),进而计算Co与H2、D2、T2反应的△H(-)、△G(-)、△S(-).CoH分子的基电子状态为三重态,Re、D(-)0、ωe分别为1.52nm、277.84 kJ/mol和1321 cm-1,与实验值基本一致.在固态分子的E和S的计算中,以气态分子计算得到的总能量中的振动能Ev代替固态能量,以总熵中的电子振动熵SEv代替固态熵.导出了Co与氢同位素气体反应的△H(-)、△G(-)、△S(-)及平衡氢压力与温度的关系.CoH的室温下平衡离解压力很低,表明CoH是一种稳定的氢化物,这与CoH分子的D(-)0很大的实验事实一致.  相似文献   

4.
用密度泛函方法B3LYP/SDD/6-311++G**计算了YH2的微观性质. 并用分子总能量中的振动能Ev代替固态能量0705212, 振动熵SEv代替固态熵的近似方法, 以及考虑到电子能量的变化, 计算了固态YH2(D, T)的焓H和熵S, 得到不同温度下Y与H2, D2, T2反应的ΔH, ΔS, ΔG及氢化反应平衡压力, 导出了与温度的依赖关系. 计算结果表明, YH2(s)的生成热为199.25 kJ•mol-1, 与实验值210.00及 225.94 kJ•mol-1非常接近, 说明近似方法的正确性.  相似文献   

5.
PuH2气态分子热力学稳定性的理论研究   总被引:6,自引:0,他引:6  
用密度泛函B3LYP方法计算了PuH2分子的微观性质、不同温度下气态PuH2分子的能量(E)、熵(S)及气态PuH2分子生成反应的标准焓变ΔH、标准熵变ΔS和标准自由能变ΔG.计算结果表明,气态PuH2分子不具有热力学稳定性.  相似文献   

6.
采用密度泛函B3P86方法和6-311++G(3df,3pf)基组,计算了在-0.05~0.05a.u.外偶极电场作用下,H2O,D2O,T2O,H2,D2,T2,O2的电子能量、核运动能量和熵值,在此基础上通过计算H2O(g)→H2(g)+O2(g)、D2O(g)→D2(g)+O2(g)、T2O(g)→T2(g)+O2(g)的焓变ΔH、熵变ΔS、Gibbs函数变化ΔG,最后得到了H2O,D2O,T2O的可逆分解电压Er.计算结果表明,外偶极电场存在时,H2O,D2O,T2O的Gibbs自由能变ΔG和可逆分解电压Er都有明显的变化,当外偶极电场正方向增加时,其Gibbs自由能变ΔG和可逆分解电压Er均趋于线性增加;当外偶极电场负方向增加时,其Gibbs自由能变ΔG和可逆分解电压Er均趋于线性减小;在相同外偶极电场作用下,Gibbs自由能变ΔG和可逆分解电压Er随H2O,D2O,T2O依次增加.  相似文献   

7.
王都留  燕翔  杨建东 《化学教育》2015,36(12):16-18
利用数轴法求解化学热力学中化学反应的吉布斯自由能变、焓变、熵变的问题, 把ΔH、T1ΔS、T2ΔS的数值或相对位置直接标在数轴上, 根据相对大小判断它们的正负号和反应的自发性。该方法既直观, 又方便、快捷, 更容易被学生理解和掌握运用。  相似文献   

8.
用量子力学B3P86方法,对H、D、T采用基函数6-311G^**,对Y采用SDD^**,计算了H2、D2、T2及其钇化合物YHn,YDn,YTn(n=1,2,3)的热力学性质,导出H与Y反应的△rHm^θ、△rSm^θ、△rGm^θ和平衡压力与温度的函数关系。文献值La-LaH2的氢化反应热为-209.296kJ/mol,本文计算值Y-YH2在298-700K间为-137.875到-155.477kJ/mol。LaH2.7的分解温度(平衡压力为0.1MPa时的平衡温度)文献值为1124℃,本文计算YH2的分解温度为782.9K。  相似文献   

9.
研究21-80℃温度范围内一些蛋白质和小分子在疏水相互作用色谱中的热行为。利用Van't Hoff作图(lnk'-1/T)测定蛋白质分子的热力学参数(ΔH°, ΔS°和ΔG°), 根据标准熵变(ΔS°)和标准自由能变(ΔG°)判断蛋白质在色谱过程中的构象变化, 通过ΔH°-ΔS°的线性关系估计蛋白质变性时的"补偿温度"(β), 鉴定蛋白质在疏水相互作用色谱中保留机理的同一性。  相似文献   

10.
王文清  闵玮   《物理化学学报》2005,21(10):1186-1194
运用统计理论热力学函数自由能ΔG、焓ΔH、熵ΔS、平衡常数K与粒子平动、振动、转动配分函数关系, 并通过变温D- 与L-CDBrClF实例计算, 证明在宏观温度变量下, 可以导致手性分子D⇔L平衡中宇称破缺熵差的反号. 根据作者科研组14年来, 采用变温X衍射、中子衍射、比热、直流和交流磁化率、1H和13C固相核磁共振、拉曼光谱、晶体旋光和双折射、超声测定相变等实验方法, 证明Salam假说预言的温度范围(200~250 K)存在温度变量诱导的相变, 产生自发对称性破缺. 在宇称破缺能差(PVED)接近0条件下, 宇称破缺熵差导致D和L分子反向的物理行为, 产生分叉机制(bifurcation mechanism). D和L分子的能量差别, 可能是早期生命起源时, L氨基酸富集的原因. 实验还发现, 在低温变温下自发对称破缺的复原. 由于晶相结构限制分子重排, Salam相变不是D→L的构型相变.  相似文献   

11.
合成了两种稀土高氯酸盐与L 脯氨酸配合物的晶体.经热重、差热、化学分析及对比有关文献,知其组成是[Pr2(L Pro)6(H2O)4](ClO4)6和[Er2(L Pro)6(H2O)4](ClO4)6,质量分数为99.24%和98.20%.选用RE(NO3)3•6H2O(RE=Pr,Er)、L Pro、NaClO4•H2O和NaNO3作辅助物,使用具有恒温环境的反应热量计,以2 mol•L-1 HCl作溶剂,分别测定了[2RE(NO3)3•6H2O+6L Pro+6NaClO4•H2O]和{[RE2(L PrO)6(H2O)4](ClO4)6+6NaNO3}在298.15 K时的溶解热.设计一热化学循环求得化学反应的反应焓ΔrHm分别是:63.904 kJ•mol-1和91.017 kJ•mol-1,经计算得配合物[RE2(L Pro)6(H2O)4](ClO4)6(s)在298.15 K时的标准生成焓ΔfHm(298.15 K)分别是-6 594.78 kJ•mol-1和-6 532.87 kJ•mol-1.  相似文献   

12.
硅烷化活性炭的吸附性质   总被引:6,自引:0,他引:6  
赵振国  樊艾星 《化学学报》1994,52(5):427-433
本工作测定了25℃和35℃时硅烷化活性炭自水溶液中吸附苯甲酸和苯甲醛的等温线;计算了吸附过程的ΔGⅲ,ΔHⅲ和ΔSⅲ;用Hill-deBoer方程处理了实验结果。所得结果表明:(1)随硅烷化时间延长,苯甲酸和苯甲醛的吸附量(mol.m^-^2)明显增加;-ΔGⅲ和-ΔHⅲ略有升高,ΔSⅲ为正值;(2)吸附分子之间的相互作用很弱,吸附分子与活性炭表面间的作用随硅烷化程度增加而加大;(3)芳香化合物可能是以苯环吸附在炭表面上的。  相似文献   

13.
Thermodynamic parameters including the equilibrium constants and enthalpy of complexation of Np(V) with oxalate at variable temperatures (T = 283-343 K, ionic strength = 1.05 mol kg(-1) NaClO(4)) were determined by spectrophotometric and microcalorimetric titrations. The results show that the complexation of Np(V) with oxalate is moderately strong and becomes weaker at higher temperatures. The complexation is exothermic and driven by both enthalpy (negative) and entropy (positive) in the temperature range from 283 K to 343 K. As the temperature is increased, both the enthalpy and entropy of complexation increase (ΔH becomes less negative and ΔS becomes more positive), having opposing effects on the complexation. Because the increase in the enthalpy (ΔH) exceeds that of the entropy term (TΔS), the complexation of Np(V) with oxalate becomes weaker at higher temperatures. The effect of temperature on the complexation is discussed in terms of the energetics of ion solvation and hydrogen bonding involved in the complexation.  相似文献   

14.
New Schiff base derivatives were prepared by the condensation of 5-chloro and 5-bromo salicylaldehyde with bis(o-aminophenol)ethers. Five bis(o-nitrophenol)ether compounds were synthesized using some ditosylate, 1,3-dibromopropane and 1,4-dibromobuthane with o-nitrophenol. These compounds were reduced to bis(o-aminophenol)ethers. The products have been characterized by elemental analysis, FTIR, 1H, 13C NMR, HETCOR and HMBC spectroscopic techniques. The tautomerisms of all of the Schiff bases compounds were determined in DMSO, CHCl3, C2H5OH and C6H12 solvents and in both acidic and basic media using the UV-vis spectrophotometric method. The heat of formation (ΔHf), enthalpy (ΔH), entropy (ΔS), Gibbs free energy (ΔGf and ΔG), stable isomers, conformations and tautomers of the synthesized compounds are calculated using the MOPAC2009 (PM6) program.  相似文献   

15.
Surface forces between gold surfaces were measured in pure water at temperatures in the range of 10-40 °C using an atomic force microscope (AFM). The surfaces were hydrophobized by self-assembly of alkanethiols (C(n)SH) with n=2 and 16 in ethanol solutions. The data were used to determine the changes in excess free energies (ΔG(f)) of the thin water films per unit area by using the Derjaguin approximation [1]. The free energy data were then used to determine the changes in excess film entropy (ΔS(f)) and the excess film enthalpy (ΔH(f)) per unit area. The results show that both ΔS(f) and ΔH(f) decrease with decreasing film thickness, suggesting that the macroscopic hydrophobic interaction involves building some kind of structures in the intervening thin films of water. It was found that |ΔH(f)|>|TΔS(f)|, which is a necessary condition for an attractive force to appear when the enthalpy and entropy changes are both negative. That macroscopic hydrophobic interaction is enthalpically driven is contrary to the hydrophobic interactions at molecular scale. The results obtained in the present work are used to discuss possible origins for the long-range attractions observed between hydrophobic surfaces.  相似文献   

16.
Photoinitiated substitution complex of [Fe(CN)6]4- with imidazole has been synthesized and characterized. On the basis of elemental analysis, the empirical molecular formula of the complex is K4[Fe(CN)5(C3H4N2)]·4H2O. The substitution of aquo ligand produced as a result of photoexcitation by imidazole has been confirmed by various spectroscopic thechniques like UV-Vis, FTIR, NMR, and SEM techniques. The characteristic FTIR and NMR ab- sorption peaks for different entities present support the assigned formul...  相似文献   

17.
氧乙烯基对胶团化过程热力学函数的影响   总被引:3,自引:0,他引:3  
利用表面张力法测定了各种条件下C_8H_(17)(OC_2H_4)_n-SO_4Na(C_8E_nS; n=0,1,3)的cmc, 并计算了胶团的反离子结合度、胶团化过程中的自由能(ΔG°)和熵变(ΔS°)。结果发现: C_8E_nS的cmc随n的增加而下降, 并且下降的幅度逐渐变小; 胶团的反离子结合度也随n的增加而减小; ΔS°随n的增加而增加, 但增加的幅度逐渐变小, 对于离子和非离子表面活性剂都是如此。人们认为这是由于氧乙烯基(EO)具有亲水和疏水二重性, 随着EO数的增加, EO的疏水性相对减弱而亲水能力将相对增加所致。EO的这个特点, 是它在表面活性剂分子中具有特殊表现的根本原因。  相似文献   

18.
噻吩加聚物(C4H4S) n(n=1~8)的密度泛函理论研究   总被引:1,自引:0,他引:1  
Thiophene polymers(C4H4S)n( n = 1 ~ 8)have been studied on B3LYP / 6-31G theory level. Vibrational frequencies,total energy(ET),zero point energy(ZPE),capacity(C0P),entropy(S0 )and energy gap(ΔE)was calculated based on the optimized equilibrium structures. By means of frequency analysis,the equilibrium structures were confirmed. The relationships between ET,ZPE,C0P,S0,ΔE and n were studied. The formation enthalpy of thiophene polymers was calculated with the total energies. The polymerized process and relative stability of the title compounds was determined according to the data of the formation enthalpy. The calculated results indicated that the thiophene molecular which has a planar structure exists in the stable chain polymers and the chain structures(C4H4S)n( n > 1)present different stabilities when n is an even or odd number. ZPE,C0P,and S0 show a linear increasing trend with n. The energy gaps ΔE show a direct proportion to n too,which indicated that the conduct property increases with n. The results also illustrated that the stepsize polymerized process is the primary way in the polymerized reactions.  相似文献   

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