变温红外确定硫氰化铵固-固相变机理(英文)

硫氰化铵分子晶体在固 固转变时 ,能可逆地吸收大量的热。作者利用变温红外光谱确定了其固 固相变机理。结果表明 ,随着温度升高 ,固 固转变时分子晶体内相邻的氢键断裂 ,晶型由低对称转变为高对称并引入振动和转动无序 ,吸收大量热。     

多元醇固-固相变的变温红外光谱研究

利用变温红外光谱技术测定了４种多元醇在４０００￣４５０ｃｍ＾－１范围内的ＩＲ光谱,分析了羟基的伸缩振动和面外变形振动随温度的变化情况,并结合ＤＳＣ对多元醇固－固相变机理进行了探讨。     

KBF4非等温固-固相变热性质的测定

利用DTA-TG和DSC热分析技术研究了无机塑晶材料KBF4固-固相变的热性能,测得转变温度为284.13℃,转变焓为105.73J/g.KBF4固-固相变的机理是随着温度的升高,晶体中离子键部分断裂,晶体逐渐由低对称的正交晶系向高对称立方晶系转变,并在这过程中,同时引入化学键的振动和转动无序,从而吸收大量的相变焓.     

多元醇及其二元混合物固-固相变的IR研究

固固相变储能物质多元醇类以其有适宜的转变温度、较高的转变焓、具有经济和技术潜力而受到人们的重视,已在热力学和动力学等方面对其进行广泛和深入的研究[1-3],并通过红外光谱法研究了几种纯多元醇固固转变的机理[1].本文对几种多元醇及其二元混合物进行变温红外光谱的测定,进一步探讨了变化的规律.1　实　验11　药品:新戊二醇(ＮＰＧ)为保证试剂(日本东京化成株式工业会社),三羟甲基乙烷(ＰＧ)超纯(日本东京化成株式工业会社),季戊四醇(ＰＥ)化学纯(北京化学试剂公司).12　仪器美国ＰＥ公司Ｍ1730型富里叶变换红外光谱仪;日本Ｅ012Ａ号Ｈ…     

PEG-沸石固-固相变材料的制备及性能

摘要：采用接枝共聚法合成了以聚乙二醇（PEG）为相变物质,沸石为骨架的PEG沸石固-固相变材料。通过红外光谱（FT—IR）、热失重分析（TGA）和差示扫描量热法（DSC）等测试手段对PEG-沸石固-固相变材料的结构、相变行为及热稳定性进行了研究。结果表明：通过改变PEG的分子量,可以得到不同相变焓和不同相变温度的PEG-沸石固-固相变材料,其相变焓可达105．41J／g,热稳定性良好,起始分解温度高于300℃。     

偏氟乙烯-四氟乙烯共聚物的β、γ混合晶型固相转变与松弛现象

本文用红外光谱及压电常数方法研究了偏氟乙烯-四氟乙烯共聚物在高压直流电场下,γ晶型向β晶型的固相转变。同时用动态力学方法、介电损耗测试法及压电常数方法研究了样品的松弛现象。     

六羟基化合物为骨架的高分子固-固相变材料的合成与性能

分别使用三种含6个羟基的化合物(山梨醇、双季戊四醇和肌醇)作为分子骨架,聚乙二醇(PEG)作为相变功能链,4,4'-二苯基甲烷二异氰酸酯(MDI)为交联剂,合成了3种具有不同交联结构的新型固-固相变储能材料。通过傅里叶变换红外光谱(FT IR)、X-射线衍射(XRD)、偏光显微镜(POM)、示差扫描量热法(DSC)和热重量分析法(TG)分别对合成材料的分子结构、结晶性能、相变行为和热稳定性进行了研究。结果显示,所制备的材料在30~70℃温度范围内具有典型的固-固相变特性,其升温和冷却过程的相变焓最高可达107.5J/g和102.9J/g。此外,通过热重分析发现所合成材料具有较好的可重复使用性和热稳定性。因此,合成的新型固-固相变材料在热能储存和控温领域具有巨大的应用潜力。     

固相反应法制备微/纳米复合相变储能材料及其测试表征

采用低热固相化学反应法制备了表面包覆SiO2的不同硬脂酸含量的复合相变储能微纳米材料.XRD分析表明所制备的相变材料均呈晶相结构,红外图谱显示复合材料包覆层SiO2与相变主体材料硬脂酸C18H36O2(SA)存在键合作用,扫描电镜图片说明所合成复合材料呈较均匀颗粒状,而差热分析则表明所制得复合相变材料的相变温度分别为66.4、64.9 ℃,相变焓分别为148.97、111.54 J/g,具有良好的蓄热能力,可用于太阳能利用等方面的储能蓄热.     

Y2O3:Eu纳米晶的硝基取代苯甲酸配合物固相热解制备和性能

以苯甲酸、邻硝基苯甲酸、间硝基苯甲酸、对硝基苯甲酸、3，5－二硝基苯甲酸等为配体制备了Y^3 、Eu^3 二元配合物，配合物中Y^3 与Eu^3 的摩尔比为9：1，利用这些配合物的爆炸式热分解特性通过固相热解反应制备了一系列Y2O3：Eu纳米晶。透射电镜观察，可以看出所得纳米晶呈球形，粒度介于40－60nm，X射线衍射分析表明实验所得纳米晶属立方晶系，粒径与电镜观察所得结果基本一致；Eu^3 的引入并不影响Y2O3的晶相组成；配体类型对纳米晶的结构没有显著影响，不过相对于硝基取代苯甲酸配合物，苯甲酸配合物热解所得Y2O3：Eu纳米晶团聚严重；退火温度显著影响纳米晶粒度，退火温度高，纳米晶粒度大，反之亦然。荧光光谱测定表明所有Y2O3：Eu纳米晶具有相似的发光行为，其中以苯甲酸配合物分解所得Y2O3：Eu纳米晶发光性能最为优越。     

二维红外光谱法分析聚酰胺-66晶区/非晶区结构

应用变温红外光谱法和二维红外光谱法对聚酰胺-66在303～393K范围内的晶区和非晶区结构及热稳定性进行研究。变温一维红外光谱和变温二阶导数红外光谱的试验结果表明,聚酰胺-66的晶区结构对温度变化较为敏感,而非晶区结构相对稳定。非晶区结构的热稳定性在二维红外光谱试验中得到进一步的证实。从聚酰胺-66的分子结构观察,随着温度的升高,其晶区结构(主要对应O=C-NH-)最先改变,而非晶区结构(主要对应-C-C-)则较为稳定。非晶区的异步二维红外光谱试验结果表明,其晶区结构的吸收波数为1 141cm-1(νamorphous-1)和1 138cm-1(νamorphous-2);而非晶区结构的吸收波数为939cm-1(νcrystal-1)和931cm-1(νcrystal-2)。对聚酰胺-66的非晶区结构和晶区结构还同时进行同步二维红外光谱试验,结果表明:随着温度的升高,两者的红外吸收峰的变化快慢顺序为931cm-1(νcrystal-2)1 141cm-1(νamorphous-1)939cm-1(νcrystal-1)1 138cm-1(νamorphous-2)。     

Temperature dependent polarized Raman spectra of nonaaqualanthanoid (Pr) single crystal

Polarized Raman spectral changes with respect to temperature were investigated for Pr(BrO3)3.9H2O single crystals. FTIR spectra of hydrated and deuterated analogues were also recorded and analysed. Temperature dependent Raman spectral variation have been explained with the help of the thermograms recorded for the crystal. Factor group analysis could propose the appearance of BrO3 ions at sites corresponding to C3v (4) and D3h (2). Analysis of the vibrational bands at room temperature confirms a distorted C3v symmetry for the BrO3 ion in the crystal. From the vibrations of water molecules, hydrogen bonds of varying strengths have also been identified in the crystal. The appearance upsilon1 mode of BrO3- anion at lower wavenumber region is attributed to the attachment of hydrogen atoms to the BrO3- anion. At high temperatures, structural rearrangement is taking place for both H2O molecule and BrO3 ions leading to the loss of water molecules and structural reorientation of bromate ions causing phase transition of the crystal at the temperature of 447 K.     

Temperature-triggered phase transition in pyridazine hexafluorophosphate

The pyndazine hexafluorophosphate[C₄H₅N₂]⁺[PF₆]^-（1） undergoes a reversible phase transition around140 K,which was confirmed by the DSC measurement.Variable-temperature crystal structures determined at 293 K and 93 K show that the compound crystallizes in the same space group P2₁/c,indicating that 1 undergoes an iso-structural phase transition.As the temperature decreases,dielectric measurement of the title compound shows no significant change around the phase transition temperature.Classic hydrogen bonds are found between molecules at 293 K and 93 l< with similar packing arrangement.The most distinct difference between the low temperature and room temperature structures is the order-disorder transition of the hexafluorophosphate anion,which is probably the driving force of the phase transition.     

Hydrogen bonded NHO chains formed by chloranilic acid (CLA) with 4,4′-di-t-butyl-2,2′-bipyridyl (dtBBP) in the solid state

In crystalline state 2,5-dichloro-3,6-dihydroxy-p-benzoquinone (chloranilic acid, CLA) forms with 4,4′-di-t-butyl-2,2′-bipyridyl (dtBBP) the hydrogen bonded chains along the b-axis. From one side of the CLA molecule the proton transfer takes place and the hydrogen bond length is very short (2.615 Å). A continuous infrared absorption is observed for dtBBP·CLA in the wavenumber range between 3100 and 800 cm⁻¹ also indicating the strong hydrogen bonds. The DSC measurements show a weak, close to continuous, phase transition at 414 K. The complex dielectric permittivity for a single crystal sample was measured in the temperature range 100-440 K and at frequencies between 200 Hz and 2 MHz. The dielectric response is a combination of semiconducting properties and a relaxation process most probably connected with the proton dynamics in the hydrogen bonds. The mechanism of the structural phase transition is discussed.     

Two-dimensional infrared spectroscopy study on phase transition and structural variations of a hydrogen-bonded liquid crystal

Infrared (IR) spectra have been measured for a liquid crystal (LC) consisting of one trans-butene diacid (BD) molecule as a proton donor and two 4-(2,3,4-tridecyloxybenzoyloxy)-4'-stilbazoles (DBS) molecules as a proton acceptor (DBS:BD:DBS) linked together with each other by inter-molecular hydrogen bonds over a temperature range from 20 to 120 degrees C to explore its phase transition and heat-induced structural variations. The temperature-dependent IR spectra have shown that the inter-molecular hydrogen bonds are stable in the liquid crystalline phase but become slightly decoupled with temperature increasing. Two kinds of two-dimensional (2D) correlation spectroscopy, variable-variable (VV) and sample-sample (SS) 2D spectroscopy, have been employed to analyze the observed temperature-dependent spectral variations more efficiently. The SS 2D correlation analysis in the spectral range of 2700-1800 cm(-1) has demonstrated that a change in hydrogen bonds in the LC starts from 40 degrees C, which is not clarified by differential scanning calorimetry (DSC) and conventional IR and Raman spectroscopic analyses. On the other hand, the phase transition of LC revealed by SS 2D spectroscopy in the specific spectral regions of 1750-1650 and 3000-2700 cm(-1) is in a good agreement with that revealed by DSC for the heating process. The VV 2D correlation spectroscopy analysis has provided information about the structural variations of inter-molecular hydrogen bonds. The different species of hydrogen-bonded and free -COOH and -COO- groups in the LC have been clarified by the VV 2D correlation analysis. It has also elucidated the specific order of the temperature-induced structural changes in the intra- and inter-molecular hydrogen bonds concerning with the -COOH and/or -COO- groups in the LC.     

月桂胺盐酸晶体相变的红外光谱研究

在290-365K的温度区间内考察了月桂胺盐酸盐晶体红外光谱随温度的变化规律。结果表明:月桂胺盐酸盐在339K发生了固-固结构相变, 该相变的预相变起始点为327K。在327K以下的低温相中, 晶体中分子的碳氢链以高度有序的全反式构象存在, 极性头部的三个N-H-Cl氢键是不等价的。在327-339K的中间过渡相, 碳氢链中出现了旁式构象, 分子链间相互作用减弱。不等价的N-H-Cl氢键的差异减小。在339K以上的高温相中, 分子旁式链构象的增多导致了分子链横向堆积无序性的明显增加, 三个N-H-Cl氢键已变得等价。     

Raman spectroscopic and DSC studies of diglycine-perchlorate (DGPCl)

Single crystals of diglycine perchlorate (DGPCl) and deuterated diglycine perchlorate (DDGPCl) are synthesized and studied using differential scanning calorimetry (DSC) and Raman spectroscopy. DSC data indicated that both DGPCl and DDGPCl undergo a reversible first-order phase transition (solid-solid) at −11.5 °C and −9.3 °C, respectively. The Raman spectra of DGPCl and DDGPCl obtained at ambient temperature are analyzed to infer on the strength of hydrogen bonding in this compound relative to the parent compounds. The occurrence of NH stretching frequency at higher value in DGPCl in comparison with glycine suggests presence of a weak N–H?O hydrogen bond in DGPCl than in glycine. The lower isotropic melting temperature of DGPCl as compared to that of glycine is understood on the basis of the relative strength of hydrogen bonding in these compounds.     

四氯合金属(II)酸烷铵在280-500K间的热力学性质和相变:III.四氯合镉(II)酸n-十二烷铵

在280-500K温度范围内用自动绝热量热计测量了(n-C~1~2H~2~5NH~3)~2CdCl~4的热容。在所研究的温度范围内发现一个固-固相转变, 其相变温度, 相变焓和相变熵分别为(332.4±0.1)K,(48.35±0.33)kJ.mol^-^1和(145.5±1.0)J.K^-^1.mol^-^1。结合已发表的(n-C~1~2H~2~5NH~3)~2MCl~4(M=Mn, Zn)的相变参数讨论了此类配合物的中心原子对其相变的影响。[MCl~4]^2^-配位方式的不同被认为是该类配合物的相变热参数产生差异的主要原因。     

Polarized vibrational studies of bisguanidinium hydrogenphosphate monohydrate

Detailed vibrational studies (FTIR and Raman on powder samples, polarized FTIR microscope on a small single crystal, polarized FTIR using Bruker reflection unit on a single crystal and polarized Raman) have been carried out. Vibrational spectra are discussed in relation to the crystal structure published previously. In this crystal a network of hydrogen bonds link water molecules, guanidinium cations and hydrogenphosphate ions. The 13 different hydrogen bonds in G2HP crystal structure are detected. On the basis of detailed vibrational studies the detailed assignment of observed bands was made. Calorimetric (DSC) studies have been performed, but no phase transition was found in the temperature range 100-350 K.     

Infrared and polarized Raman spectra of (CH3)2NH2Al(SO4)2 x 6H2O

FTIR and single crystal Raman spectra of (CH3)2NH2Al(SO4)2 x 6H2O have been recorded at 300 and 90 K and analysed. The shifting of nu1 mode to higher wavenumber and its appearance in Bg species contributing to the alpha(xz) and alpha(yz) polarizability tensor components indicate the distortion of SO4 tetrahedra. The presence of nu1 and nu2 modes in the IR spectrum and the lifting of degeneracies of nu2, nu3, and nu4 modes are attributed to the lowering of the symmetry of the SO4(2-) ion. Coincidence of the IR and Raman bands for different modes suggest that DMA+ ion is orientationally disordered. One of the H atoms of the NH2 group of the DMA+ ion forms moderate hydrogen bonds with the SO4(2-) anion. Al(H2O)6(3+) ion is also distorted in the crystal. The shifting of the stretching modes to lower wavenumbers and the bending mode to higher wavenumber suggest that H2O molecules form strong hydrogen bonds with SO4(2-) anion. The intensity enhancement and the narrowing of nu1SO4, deltaC2N and Al(H2O)6(3+) modes at 90 K confirm the settling down of the protons in the hydrogen bonds formed with H2O molecules and NH2 groups. This may be one of the reasons for the phase transition observed in the crystal.