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1.
利用密度泛函理论并结合改进的基本度量理论研究了球形微腔中AaDd型氢键流体的相态结构.首先,根据氢键流体在球腔中的吸附-脱附等温线以及相应的巨势等温线获得不同条件下氢键流体的相图.在此基础上,重点讨论了氢键作用、球腔尺寸以及腔壁与流体之间的相互作用等因素对氢键流体相平衡特征的影响.结果表明,流体层化转变和毛细凝聚的临界温度、临界密度和临界相区域等相态特征与这些因素密切相关.研究结果可为进一步揭示几何约束下氢键流体的相平衡及聚集态结构提供可能的理论线索.  相似文献   

2.
利用密度泛函理论并结合改进的基本度量理论研究了球形微腔中AaDd型氢键流体的相态结构.首先,根据氢键流体在球腔中的吸附一脱附等温线以及相应的巨势等温线获得不同条件下氢键流体的相图.在此基础上,重点讨论了氢键作用、球腔尺寸以及腔壁与流体之间的相互作用等因素对氢键流体相平衡特征的影响.结果表明,流体层化转变和毛细凝聚的临界温度、临界密度和临界相区域等相态特征与这些因素密切相关.研究结果可为进一步揭示几何约束下氢键流体的相平衡及聚集态结构提供可能的理论线索.  相似文献   

3.
水介质中氢键吸附与疏水吸附协同作用的研究   总被引:7,自引:0,他引:7  
研究了丙烯酸型树脂(D152)在水、乙醇和正己烷中对苯胺、N-甲基苯胺和N,N-二甲基苯胺的吸附行为.在水中D152树脂对3种吸附质的吸附亲合性随N上甲基数的增加而增大,说明疏水作用是主要的吸附机理,但其吸附焓己超出范德华力的范围而在氢键的键能范围内,故氢键吸附也同时在起作用.在正己烷中,D152树脂对3种吸附质的吸附亲合性随N上甲基数的增加而减小,与水中呈相反的趋势,说明氢键作用是主要的吸附机理.在乙醇中,D152树脂对3种吸附质均无吸附,因为疏水作用和氢键作用均受到的乙醇抑制.在水中,吸附质与树脂间的氢键作用同样受到水的抑制,但氢键吸附却依然存在,说明水介质中氢键吸附和疏水吸附可能存在一种协同作用.在热力学上对水介质中氢键吸附和疏水吸附的协同作用给于合理的解释.  相似文献   

4.
Janus粒子在结构和性质上的特殊性使其在不同溶剂中呈现出丰富的聚集态结构和相态结构,这与其在溶液中的过量熵密切相关.本文以Janus粒子与氢键流体的稀溶液体系为例,利用经典流体的密度泛函理论研究了氢键流体中Janus粒子的过量熵.首先在极稀条件下给出Janus粒子外氢键流体中的局域密度分布,由此得到Janus粒子与氢键流体的二体分布函数,进而计算了不同情况下的过量熵.在此基础上,阐明了Janus粒子与氢键流体间的相互作用、氢键流体的体相密度、氢键强度和氢键官能度等因素对过量熵的影响.本研究旨在揭示这些因素对过量熵的调控机制,在定量水平上明确Janus粒子在溶液中组装的驱动力,从而为深入研究其聚集态结构提供可借鉴的理论线索.  相似文献   

5.
提出了一种通过乳化剂复配简便制备表面包覆率可调的核-壳复合微球的方法.高效液相色谱和zeta电位测试结果表明,核粒子和壳粒子在分散混合过程中出现了乳化剂吸附和脱附的再平衡现象,从核粒子表面游离的阳离子乳化剂与壳粒子表面的阴离子乳化剂发生电性中和作用,导致核、壳2种粒子的zeta电位值互相接近,基于静电作用的异相凝聚失效.进一步研究发现,在保持核粒子分散液中乳化剂总量为1 wt%的前提下,添加非离子乳化剂既可以确保分散体系的稳定性,又可以调控阳离子乳化剂的游离量,成功实现核-壳复合微球的异相凝聚.由此可见,通过调节复配乳化剂中阳离子与非离子乳化剂的配比,可简便地调控复合微球的表面包覆率.还探讨了异相凝聚体系中pH值和电解质浓度对核-壳复合微球表面包覆率的影响.  相似文献   

6.
AaDd型氢键流体的统计理论(Ⅰ): 几何相变   总被引:1,自引:0,他引:1       下载免费PDF全文
王海军 《中国科学B辑》2006,36(3):211-217
通过两种不同的统计方法研究了AaDd型氢键体系中的氢键对体系的一些物理化学特征的影响. 指出获得氢键簇合物数量分布函数的两种新方法, 得到该体系的平衡自由能以及氢键度与外界条件之间关系的解析表达式, 讨论了氢键的成键概率与相关热力学量的关系. 在平均场理论的框架下, 证明了非线性氢键体系中发生的溶胶-凝胶相转变是一类几何相变, 而非热力学相变. 进一步对氢键体系中此类几何相变与液-固热力学相变间的关系进行了初步探讨.  相似文献   

7.
构造了高岭石硅氧层和铝氧层的团簇模型(分别为Si13O37H22和Al6O24H30), 并分别在B3LYP/6-31G(d), MP2/6-31G(d)//B3LYP/6-31G(d)和B3LYP/6-311++G(d,p)//B3LYP/6-31G(d)理论水平上对1,3,5-三硝基苯(TNB)在高岭石表面的吸附性质(如优化的几何构型、 结构参数、 吸附能、 振动频率、 静电势和分子轨道等)进行了研究. 结果表明, TNB和硅氧层表面间的相互作用以静电和范德华相互作用为主; TNB与铝氧层间的相互作用以氢键为主, 且TNB和铝氧层间相互作用的能量更低, 结构更稳定.  相似文献   

8.
王海军 《中国科学B辑》2006,36(5):372-378
应用统计力学原理对AaDd型氢键流体的状态方程进行研究, 讨论了氢键的形成对于体系体积的影响, 指出氢键数量对于状态方程的修正. 然后将整个体系分成多个子系统, 并研究了子系统内分子数密度和氢键数密度的涨落以及涨落的空间关联性. 进一步给出体系中“分子-氢键”数密度相关函数与分子数密度相关函数和氢键数密度相关函数三者之间的约束方程. 作为应用, 以 van der Waals 氢键流体为例, 讨论了氢键对此类流体状态方程的影响.  相似文献   

9.
10.
应用自洽场理论(SCFT)研究了受限于球内的高分子溶液的结构,重点关注高分子链在受限壁附近的行为.根据自洽场理论数值计算结果,讨论了球半径、高分子与球限制壁的相互作用、高分子平均浓度等因素对球内高分子浓度分布的影响.从高分子浓度分布和吸附/排空层厚度可以发现,在一定的条件下,受限的高分子在受限壁上会发生吸附/排空转变.吸附/排空转变与受限球大小、高分子链长和平均浓度,以及高分子链与受限壁之间相互作用都有关系.理论预测发生吸附/排空转变时的高分子与球限制壁的临界相互作用参数与链长的倒数成线性关系,且斜率与球半径有关.限制球越小,要发生吸附/排空转变,需要高分子与球之间有更大的临界吸引能.  相似文献   

11.
Phase equilibria of hydrogen bonding (HB) fluid confined in a slit pore with broken symmetry were investigated by the density functional theory incorporated with modified fundamental measure theory, where the symmetry breaking originated from the distinct interactions between fluid molecules and two walls of the slit pore. In terms of adsorption-desorption isotherms and the corresponding grand potentials, phase diagrams of HB fluid under various conditions are presented. Furthermore, through phase coexistences of laying transition and capillary condensation, the effects of HB interaction, pore width, fluid-pore interaction and the broken symmetry on the phase equilibrium properties are addressed. It is shown that these factors can give rise to apparent influences on the phase equilibria of confined HB fluid because of the competition between intermolecular interaction and fluid-pore interaction. Interestingly, a significant influence of broken symmetry of the slit pore is found, and thus the symmetry breaking can provide a new way to regulate the phase behavior of various confined fluids.  相似文献   

12.
The vapor–liquid equilibria of binary polymer–solvent systems was modeled using the Non-Random Hydrogen Bonding (NRHB) model. Mixtures of poly(ethylene glycol), poly(propylene glycol), poly(vinyl alcohol) and poly(vinyl acetate) with various solvents were investigated, while emphasis was put on hydrogen bonding systems, in which functional groups of the polymer chain can self-associate or cross-associate with the solvent molecules. Effort has been made to explicitly account for all hydrogen bonding interactions. The results reveal that the NRHB model offers a flexible approach to account for various self- or cross-associating interactions. In most cases model's predictions (using no binary interaction parameter kij = 0) and model's correlations (using one temperature independent binary interaction parameter, kij ≠ 0) are in satisfactory agreement with the experimental data, despite the complexity of the examined systems.  相似文献   

13.
The calculations for a water‐acetonitrile‐substituted phenols system and the comparison with the experimental parameters will be given. Here we study change in the nature of the interactions into the system with donor and acceptor electron substituents on the phenolic ring, the structures, relative energies and harmonic frequencies. The conformers showed a significant difference in the OH and CN band shift depending on the type of the hydrogen bond formed and the position of the substituent on the phenolic ring. The cyclical hydrogen bonds between water‐acetonitrile and substituted phenol OH are important evidence of the relative stability in the system under study.  相似文献   

14.
N-Protonated amides have been proposed as intermediates in several biologically important reactions, but they have yet to be identified spectroscopically. The first step toward this goal is now reported in the form of spectroscopic and crystallographic proof of a strong intramolecular hydrogen bond between a charged proton donor and an amide nitrogen atom in the “proton sponge” derivative 1 ; novel reactivity results from this interaction. TfO−=trifluoromethanesulfonate.  相似文献   

15.
The geometric structures, infrared spectra and hydrogen bond binding energies of the various hydrogen‐bonded Res?‐water complexes in states S0 and S1 have been calculated using the density functional theory (DFT) and time‐dependent density functional theory (TD‐DFT) methods, respectively. Based on the changes of the hydrogen bond lengths and binding energies as well as the spectral shifts of the vibrational mode of the hydroxyl groups, it is demonstrated that hydrogen bonds HB‐II, HB‐III and HB‐IV are strengthened while hydrogen bond HB‐I is weakened in the four singly hydrogen‐bonded Res?‐Water complexes upon photoexcitation. When the four hydrogen bonds are formed simultaneously between one resorufin anion and four water molecules in the Res?‐4Water complex, all the hydrogen bonds are weakened in both the ground and excited states compared with those in the corresponding singly hydrogen‐bonded Res?‐Water complexes. Furthermore, in complex Res?‐4Water, hydrogen bonds HB‐II and HB‐IV are strengthened while hydrogen bonds HB‐I and HB‐III are weakened after the electronic excitation. The hydrogen bond strengthening and weakening in the various hydrogen‐bonded Res?‐water complexes should be due to the redistribution of the charges among the four heteroatoms (O1‐3 and N1) within the resorufin molecule upon the optical excitation.  相似文献   

16.
在B3LYP/6-31+G**//HF/6-31+G**水平上研究了在不同电场极化环境下碱基对A-T的几何构型和电子结构. 通过碱基对的氢键和结合能的变化讨论了碱基对间的质子转移, 进一步利用密度泛函理论结合非平衡态格林函数方法研究了通过碱基对的电子输运行为. 结果表明, 在0.6~2.0 V的偏压下, 由T向A方向的电子传递更易进行, 表现了微弱的整流行为.  相似文献   

17.
The intermolecular hydrogen bonds of mono‐ and dihydrated complexes of 7‐(3′‐Pyridyl)indole (7‐3′PI) have been investigated using the time‐dependent density functional theory (TD‐DFT) method. The electrostatic potential analysis of monomer 7‐3′PI and 7‐(3′‐Pyridyl)indole‐water (7‐3′PI‐W) indicates that an intermolecular hydrogen bond between two waters can be formed for 7‐(3′‐Pyridyl)indole‐2water (7‐3′PI‐2W) complex. The calculated bond lengths of the intermolecular hydrogen bonds of 7‐3′PI‐W and 7‐3′PI‐2W in the S1 state (the first excited singlet state) are all shortened compared to the ground state. By the analysis of bond length, charge population and infrared spectra, it is demonstrated that the intermolecular hydrogen bonds of 7‐3′PI‐W and 7‐3′PI‐2W are all strengthened upon electronic excitation to the S1 state. Moreover, the fluorescence of 7‐3′PI‐W and 7‐3′PI‐2W are all red‐shifted to larger wavelength compared to monomer 7‐3′PI. The red‐shift of fluorescence peak of 7‐3′PI‐W and 7‐3′PI‐2W should be attributed to the change of hydrogen bond interaction before and after photoexcitation. Therefore, it can be concluded that the intermolecular hydrogen bonding strengthening in the excited S1 state induces the fluorescence weakening of 7‐3′PI.  相似文献   

18.
This work reveals the influence of pendant hydrogen bonding strength and distribution on self-assembly and the resulting thermomechanical properties of A-AB-A triblock copolymers. Reversible addition-fragmentation chain transfer polymerization afforded a library of A-AB-A acrylic triblock copolymers, wherein the A unit contained cytosine acrylate (CyA) or post-functionalized ureido cytosine acrylate (UCyA) and the B unit consisted of n-butyl acrylate (nBA). Differential scanning calorimetry revealed two glass transition temperatures, suggesting microphase-separation in the A-AB-A triblock copolymers. Thermomechanical and morphological analysis revealed the effects of hydrogen bonding distribution and strength on the self-assembly and microphase-separated morphology. Dynamic mechanical analysis showed multiple tan delta (δ) transitions that correlated to chain relaxation and hydrogen bonding dissociation, further confirming the microphase-separated structure. In addition, UCyA triblock copolymers possessed an extended modulus plateau versus temperature compared to the CyA analogs due to the stronger association of quadruple hydrogen bonding. CyA triblock copolymers exhibited a cylindrical microphase-separated morphology according to small-angle X-ray scattering. In contrast, UCyA triblock copolymers lacked long-range ordering due to hydrogen bonding induced phase mixing. The incorporation of UCyA into the soft central block resulted in improved tensile strength, extensibility, and toughness compared to the AB random copolymer and A-B-A triblock copolymer comparisons. This study provides insight into the structure-property relationships of A-AB-A supramolecular triblock copolymers that result from tunable association strengths.  相似文献   

19.
The crystal structure of the title compound was determined (crystal data at 143 K: triclinic, space group P−1, Z=4, a=9.538(2) Å, b=11.638(2) Å, c=14.473(2) Å, α=88.647(3)°, β=89.875(3)°, γ=83.835(3)°, V=1596.9(4) Å3). In the crystal there exist two kinds of tetrameric O–HO hydrogen-bond (H-bond) systems that are quite similar to each other. The oxygen atoms accept also intermolecular C–HO H-bonds. The two types of the H-bonds connect the molecules to an infinite two-dimensional supramolecular unit, the stacking of which is aided by an intermolecular C–Hπ H-bond. A phase transition with ΔHt=4.4±0.1 kJ/mol was found at around 420 K.  相似文献   

20.
利用溶胶-凝胶分配理论对氢键溶液的模型体系进行研究, 给出了体系的凝胶化条件以及凝胶点后氢键网络中各类结构参数的计算方案, 并进行了相应的数值计算. 结果表明, 当两类质子受体基团的活性不同时, 质子受体基团的竞争作用对网络结构有一定影响. 这为控制氢键网络结构特征提供了可能的理论线索.  相似文献   

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