铝含量对LaNi_(5-x)Al_x合金氘化与去氘化动力学函数的影响

测定了LaNi5 -xAlx(x =0 ,0 1,0 2 ,0 3 )的氘化与去氘化的动力学参数 ,评价了铝含量对LaNi5 -xAlx 合金的氘化与去氘化动力学函数的影响。研究结果表明 ,铝含量不改变合金的氘化与去氘化的反应级数 ;反应速率常数随x的增加而减少 ;活化能随x的增加而增加 ;氘化与去氘化反应级数a (由气相氘压决定 )和b (由固相氘浓度决定 )分别为 2和 1及 0 5和 1。在α β相域 ,氘化与去氘化反应的速控步骤分别为氘化物的成核 长大过程和氘化物中氘的扩散过程     

LaNi5-xAlx合金吸放氢过程的滞后现象

测定了LaNi5-xAlx(x=0, 0.1, 0.2, 0.3)合金在吸放氢过程中P-C等温线的坪台压力及热力学参数.结果表明,坪台压力与热力学参数焓变ΔH,熵变ΔS随合金中Al含量的增加而降低,吸氢及放氢过程中的坪台压力存在一定的差异,即滞后现象(用滞后系数Hf表示).Hf随温度的升高而减弱,随合金中Al含量的增加而降低.滞后现象与合金在吸放氢过程中的应力释放有关.     

铝含量对LaNi5—xAlx合金氘化与去氘化动力学函数的影响

测定了LaNi5-xAlx(x=0,0.1,0.2,0.3)的氘化去氘化的动力学参数,评价了铝含量对LaNi5-xAlx合金的氘化与去氘化动力学函数的影响,研究结果表明,铝含量不改变合金的氘化与去氘化的反应级数;反应速率常数随x 的增加而减少,活化能随x的增加而增加,氘化与去氘化反应级数a和b(由固相氘浓度决定）分别为2和1及0．5和1O在α β相域,氘化与去氘化反应的速控步骤分别为氘化物的成核－长大过程和氘化物中氘的扩散过程。     

Cr-Ni二元相图

利用X射线衍射、电子探针微分析、扫描电子显微镜和差热分析测定了Cr-Ni合金样品和扩散偶Cr-Ni样品,构筑了Cr-Ni二元体系的相图.在此相图中存在、 γ和α相，这些相的结构分别属于A2, A1和型结构.它们的晶胞参数分别随着温度的增加和Cr含量的增加而增大.温度变化对晶胞参数的影响强于Cr含量变化对晶胞参数的影响.δ相仅存在于未退火的熔炼样品中和差热分析后的样品中.该相属于不稳定相.     

镁含量对RE-Mg-Ni系A2B7型储氢合金结构与性能的影响

采用感应熔炼方法制备了La0.8-xGd0.2MgxNi3.1Co0.3Al0.1(x=0, 0.1, 0.15, 0.2, 0.25, 0.3, 0.4)储氢合金, 并在氩气气氛和1173 K下进行退火处理. 合金相结构分析结果表明, 镁含量(x)较低时合金以Ce2Ni7型为主相结构, A2B7型相丰度(Ce2Ni7+Gd2Co7)达到98.8%; 镁含量较高时合金相由A2B7型、 CaCu5型和PuNi3型物相构成, 随着镁含量的增加, PuNi3型和CaCu5型相组成逐渐增多, 其晶胞参数随Mg含量的增加而减小, 同时合金的吸氢平台也随之升高. 电化学测试结果表明, 随着合金中Mg含量增加, 合金电极的最大放电容量和循环稳定性均呈先增大后减小的规律, 其中x=0.15时合金电极具有最高的电化学放电容量(393 mA·h/g)和最佳的循环寿命(S100=92.82%). 合金电极的高倍率放电性能(HRD)随Mg含量的增加先减小再增大然后又减小, 适量的Mg元素改善了合金电极的动力学性能.     

La-Mg-Ni系A2B7型贮氢合金的结构与电化学性能

合金结构研究表明,La2-xMgxNi7(x=0.3～0.8)主要由Ce2Ni7,Gd2Co7,PuNi3型物相组成.合金中Mg含量对合金相结构有着重要影响,主相的晶胞参数随Mg含量(x)的增加呈线性减小,合金的吸放氢平台也随之升高.电化学测试表明,随合金中Mg含量的增加,合金电极的放电容量先增大后减小,合金电极的循环稳定性呈恶化趋势,La1.4Mg0.6Ni7合金电极具有最高的电化学放电容量(378 mAh·g-1),La1.6Mg0.4Ni7合金电极具有最佳的循环稳定性(S270=81%).合金电极的高倍率放电性能(HRD)随Mg含量的增加而增大.当合金中Mg含量较低时(x≤0.5),合金电极反应速度控制步骤为氢在合金体相中的扩散;当Mg含量较高时(x≥0.5),合金电极反应速度控制步骤转变为电极表面的电荷转移.     

钪元素对AB2型合金Zr1-xScxMn0.6V0.2Ni1.2Co0.1（x=0～1）储氢和电化学性能的影响

用真空电弧熔炼方法制备了Zr1-xScxMn0.6V0.2Ni1.2Co0.1(x=0～1)AB2型储氢合金,研究了Sc元素替代Zr对合金的微观组织结构、气态储氢及电化学性能的影响。研究结果表明,Zr1-xScxMn0.6V0.2Ni1.2Co0.1合金主要是由FCC型C15相、CsCl型结构的(ScZr)Ni相和少量的Ni10Zr7相组成,随Sc含量的增加,C15相丰度逐渐减小,(ScZr)Ni相丰度逐渐增加,当x=0.2时Ni10Zr7相基本消失;Sc元素对合金的首次气态吸氢动力学行为影响较大,随Sc含量的增加,合金吸氢动力学性能逐渐变缓,但吸氢容量逐渐提高,直至达x=1.0时的最大吸氢量1.87%;Sc元素对合金吸氢PCT曲线平衡氢压的影响规律不明显,随Sc含量增加,合金氢化物的形成焓ΔH从-26.66 kJ.mol-1逐渐减小到-8.14 kJ.mol-1。Sc元素的加入可明显改善合金电极的活化性能,提高放电容量,随Sc含量的增加,合金电极最大放电容量从x=0时的350.3 mAh.g-1增加到x=1时的429.8 mAh.g-1,呈先减小后增大的趋势,但电极容量的保持率S100随Sc含量增加而快速下降。     

铜模吸铸Nd9Fe83-xTi4C4Bx（x=1015）合金组织演化和磁性能的研究

采用铜模吸铸及随后的退火处理制备了厚度为0.8 mm,成分为Nd9Fe83-xTi4C4Bx(x=10~15)的Nd2Fe14B/Fe3B型纳米复相磁体,对其组织演变和磁性能进行了研究。结果表明:在铸态合金中,x=10的合金微观组织主要由Nd2Fe14B,Fe3B,α-Fe和TiC相构成。而x=11~15的合金中除含上述各相外,还出现了Nd2Fe23B3相、未知相和非晶相,且随着B含量的增加,它们在合金中的相对含量有不同程度的增加;退火过程中,随着合金中亚稳相和非晶相的转化,Nd2Fe14B,Fe3B和α-Fe相对含量增加,但不同B含量合金的相结构变化差异明显,导致退火后磁体具有不同的磁性能。其中,x=12的合金在680℃退火5 min后获得了最佳磁性能:Br=0.63 T,iHc=98.12 kA·m-1,(BH)max=22.79 kJ·m-3。     

Mg_2Ni_(1-x)Co_x合金相的固溶烧结法制备及结构和储氢性能

采用固溶烧结法制备了Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金,利用X射线衍射仪和压力-组成-温度测试仪等研究了Co含量对合金相结构和储氢性能的影响.结果表明,合金由Mg_2Ni型Mg_2(Ni,Co)主相及少量Mg和Mg Ni3Co新相组成.Mg2(Ni,Co)具有良好的可逆储氢性能,吸氢形成Mg_2Ni_(0.9)Co_(0.1)H_4型四元氢化物,其具有与父系氢化物HT-Mg_2NiH_4相近的放氢焓变(ΔHd=63.9 k J/mol H2).Mg_2Ni_(1-x)Co_x(x=0.10,0.15,0.20)合金具有良好的放氢动力学性能,二维相界面迁移为放氢过程的控制步骤.随着Co含量的增加,合金的放氢活化能(Ea)降低,其中,Mg_2Ni_(0.8)Co_(0.2)的Ea降低到54.0 k J/mol.     

La0.8-xPrxMg0.2Ni3.2Co0.4Al0.2(x=0～0.4)储氢合金的相结构与电化学性能

研究了Pr替代La对La0．8-xPrxMg0．2Ni3．2Co0．4Al0．2（X=0～0．4）储氢合金相结构与电化学性能的影响。XRD及Rietveld全谱拟合方法分析表明，合金主要由PrsCo-9，Ce5Co-9及CaCu5型物相组成。随着Pr含量x值的增加，合金中A5B19型物相（Pr5Co19＋Ce5Co19）逐渐增多，同时各物相的晶胞参数（a，c）和晶胞体积（y）均减小。电化学测试表明，x值的增加对合金电极的活化性能影响不大，但可显著提高合金电极的循环稳定性。合金的高倍率放电性能（HRD）随着x的增加呈增加趋势，在x=0．3时存在最大值（HRD900=89．6％）；合金电极的HRD主要由合金电极表面的电荷迁移速率所控制。     

Combination of the Metropolis Monte Carlo and Lattice Statics method for geometry optimization of H‐(Al)‐ZSM‐5

In this article, the combination of the Metropolis Monte Carlo and Lattice Statics (MMC‐LS) method is applied to perform the geometry optimization of crystalline aluminosilicate zeolite system in the presence of cationic species (H⁺), i.e., H‐(Al)‐ZSM‐5. It has been proved that the MMC‐LS method is very useful to allow H⁺ ions in (Al)‐ZSM‐5 extra‐framework to approach the global minimum energy sites. The crucial advantage of the combination MMC‐LS method is that, in stead of simulating over thousands random configurations via the only LS method, the only one configuration is needed for the MMC‐LS simulation to achieve the lowest energy configuration. Therefore, the calculation time can be substantially reduced via the performance of the MMC‐LS method with respect to the only LS method. The calculated results obtained from the MMC‐LS and the only LS methods have been comparatively represented in terms of the thermodynamic and structural properties. © 2010 Wiley Periodicals, Inc. J Comput Chem 2010     

Lattice sum calculations for 1/rp interactions via multipole expansions and Euler summation

A method is developed here for doing multiple calculations of lattice sums when the lattice structure is kept fixed, while the molecular orientations or the molecules within the unit cells are altered. The approach involves a two‐step process. In the first step, a multipole expansion is factored in such a way as to separate the geometry from the multipole moments. This factorization produces a formula for generating geometry constants that uniquely define the lattice structure. A direct calculation of these geometry constants, for all but the very smallest of crystals, is computationally impractical. In the second step, an Euler summation method is introduced that allows for efficient calculation of the geometry constants. This method has a worst case computational complexity of O(( log N)²/N), where N is the number of unit cells. If the lattice sum is rapidly converging, then the computational complexity can be significantly less than N. Once the geometry constants have been calculated, calculating a lattice sum for a given molecule becomes computationally very fast. Millions of different molecular orientations or molecules can quickly be evaluated for the given lattice structure. © 2000 John Wiley & Sons, Inc. J Comput Chem 22: 208–215, 2001     

铕掺杂TiO2的制备及其可见光光催化性能研究

采用溶胶-凝胶法制备了不同铕(Eu)掺杂量的TiO₂纳米颗粒(Eu-TiO₂),利用透射电镜(TEM),X射线光电子能谱(XPS),X射线衍射(XRD)及紫外可见漫反射(UV-Vis DRS)等方法对Eu-TiO₂进行了物理特性的初步表征.结果表明:与未掺杂纳米TiO₂比较,Eu-TiO₂禁带宽度变窄,具有可见光光催化活性.在可见光下(λ≥420 nm)照射下,以光催化降解染料罗丹明B(Rhodamine B,RhB)为目标反应,探讨了Eu-TiO₂不同制备条件对RhB降解光催化活性的影响,优化得到制备高活性Eu-TiO₂最佳pH为3、掺杂比例(n_Eu/n_Ti)为0.05%、煅烧温度为500 ℃.研究了可见光照射下Eu-TiO₂降解RhB和无色有机小分子水杨酸(SA)光催化反应条件及降解特性,RhB的12 h深度氧化矿化率为60.2%,SA的8 h降解率达到100%.通过跟踪测定可见光下Eu-TiO₂光催化反应过程中氧化物种的变化,研究了可见光激发Eu-TiO₂光催化反应机理,表明其光催化反应主要涉及羟基自由基(·OH)历程.     

Electron pairing in one‐dimensional anharmonic crystal lattices

We show that when anharmonicity is added to the electron–phonon interaction it facilitates electron pairing in a localized state. Such localized state appears as singlet state of two electrons bound with the traveling local lattice soliton distortion, which survives when Coulomb repulsion is included. © 2011 Wiley Periodicals, Inc. Int J Quantum Chem, 2012     

Lattice energy of organic ionic crystals and its importance in analysis of features,behaviour and reactivity of solid-state systems

A general approach to the theoretical evaluation of the crystal lattice energy of ionic substances, particularly those composed of monoatomic ions, is outlined in detail. Subsequently, the possibilities of theoretical prediction of the lattice energy of complex organic and inorganic ionic substances are discussed. Lastly, the importance of the lattice energy in examinations of the properties and behaviour of solid-state systems, is treated, together with the prospects of developing a model describing the kinetics of solid-state processes.The financial support of this work by the Polish State Committee for Scientific Research (KBN) under grant no. DS/5-300-7-016-1 is gratefully acknowledged.     

IR-active lattice modes of α-glycine and deutero-α-glycine

The 9 IR-active lattice modes of alpha-glycine have been observed in the far-infrared using a Fourier transform Michelson interferometer.     

Effect of molecular orientation distribution and crystallinity on the measurement of the crystal lattice modulus of nylon 6 by x-ray diffraction

The crystal lattice modulus of nylon 6 (-type) was measured by x-ray diffraction using nylon 6 films drawn up to five times. The measured crystal lattice modulus was 173–175 GPa for all specimens whose crystallinity and the Young's modulus were beyond 46% and 3.75 GPa, respectively. These results indicate that a state of homogenous stress can be achieved. In contrast, the values were scattered for the speciments whose crystallinity and Young's modulus are less than the above values. To study the origin, a numerical calculation of the crystal lattice modulus, as measured by x-ray diffraction, was carried out by considering effects on the orientation factors of molecular chains and crystallinity. In this calculation, a previously introduced model was employed, in which oriented crystalline layers are surrounded by oriented amorphous phases so that the strains of the two phases at the boundary are identical. The theoretical results calculated by the introduced model indicated that the crystal lattice modulus by x-ray diffraction is almost equal to the intrinsic crystal modulus if the morphology of the test specimen can be represented as a series model. In contrast, if a parallel model is more appropriate, the difference between the measured modulus and the intrinsic value can be pronounced. Such morphological dependence was found to be less pronounced with increasing high degree of molecular orientation and crystallinity.     

Hydrophobicity‐Driven Self‐Assembly of an Eighteen‐Membered Honeycomb Lattice with Almost Classical Spins

The design and synthesis of model compounds that do not exist naturally is one of the important targets in modern coordination chemistry. Herein, an eighteen‐membered honeycomb structure with equal numbers of Mn^II (s=5/2) and Gd^III (s=7/2) metal centers has been prepared, for the first time, by using a hydrophobic force‐directed self‐assembling process. Due to the weakly coupled Gd^III pairs, the magnetic properties are mainly determined by eight‐membered chains in the experimentally considered temperature range. These [Mn₄Gd₄] ”finite‐size“ chains, albeit with large Hilbert space, can be fully resolved by the high‐temperature series expansion and the powerful finite‐temperature Lanczos method, which reveal that the exchange‐couplings between the metal centers are antiferromagnetic and consistent with the magnetization measurement. Interestingly, from the surface‐engineering point of view, the [Mn₄Gd₄] chains are ”precisely“ assembled into a 2D honeycomb pattern, which is potentially desirable in the design of weakly coupled qubits.     

General analysis of the measurements of the lateral crystal lattice moduli of semicrystalline polymers by x-ray diffraction and the application to nylon 6

A mathematical representation based on a linear elastic theory is proposed by which one may investigate the dependences of molecular orientation and crystallinity on the crystal lattice moduli and linear thermal expansion coefficients in the direction perpendicular to the chain axis as commonly measured by x-ray diffraction. In the theoretical calculation, a previously introduced model was employed in which oriented crystalline phase is surrounded by oriented amorphous phase and the strains of the two phases at the boundary are identical. The mathematical analysis indicated that the lateral crystal lattice moduli and linear thermal coefficients as measured by x-ray diffraction may be different from the intrinsic crystal moduli and linear thermal coefficients of a crystal unit cell, depending on the structure of the polymer solid. The numerical calculation was applied to nylon 6. As a result, it may be confirmed that the lateral crystal lattice moduli measured by x-ray diffraction are sensitive to the morphology of the bulk speciments and close to the intrinsic crystal moduli if the morphology of the test specimen can be represented by a parallel model with respect to the original stretching longitudinal direction.     

Helical Structures: The Geometry of Protein Helices and Nanotubes

In nature, helical structures arise when identical structural subunits combine sequentially, the orientational and translational relation between each unit and its predecessor remaining constant. A helical structure is thus generated by the repeated action of a screw transformation acting on a subunit. A plane hexagonal lattice wrapped round a cylinder provides a useful starting point for describing the helical conformations of protein molecules, for investigating the geometrical properties of carbon nanotubes, and for certain types of dense packings of equal spheres.