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。     

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

在280-500K的温度范围内用自动绝热量计测定了(n-C12HxNH3)2MnCl4的热容.发现了两个固-固相变,固ID→固II和固I→固II.前者的相变温度、相变焓和相变熵分别为330.6±0.1K,47.78±0.29kJ.mol^-^1和144.5±0.9J.K^-^1.mol^_^1,后者的对应相变热参数分别为334.5±0.1K,5.96±0.05kJ.mol^-^1和17.82±0.15J.K^-^1.mol^-^1.报道了该物质每隔10K的热力学性质.     

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_(12)H_(25)NH_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_(12)H_(25)NH_3)_2MCl_4(M=Mn,Zn)的相交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。     

四氯合锌酸二(正十一烷基铵)晶体相变的Raman光谱

用Raman光谱研究了[n-C~11H~23NH~3]~2ZnCl~4(简记为C~nZn)配合物的固-固相变。结果表明, 配合物产生的固-固相变主要与烷烃链的堆积结构和分子构象变化有关, 在T~cl=25℃的相变是由于烷烃链的侧向堆积和分子构象的有序到部分无序变化。在中间相, 分子链局部产生旁式构象。在T~c2=87℃的相变主要来源于烷烃链从部分构象有序到完全无序的变化, 高温相形成了构象完全无序相, 相应于烷烃链的"熔化"。     

四氯合金属(II)酸正烷铵在280-500K间的热力学性质和相变 II: 四氯合锌(II)酸正十二烷铵

研究了四氯合锌(II)酸正十二烷铵(C12H25NH3)2ZnCl4(1)]在280-500K间的热力学性质和相变热参数. 据报导(RNH3)MX4型化合物在300-380K间有相变焓很大的固-固相变, 是很有开发前景的固-固相变低温储能材料, 本文为(1)的应用提供了精确的热数据.     

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

在280-500K的温度范围内用自动绝热量热计测定了(n-C_(12)H_(25)NH_2)_2MnCl_4的热容。发现了两个固-固相变,固_(Ⅲ)→固_(Ⅱ)和固_Ⅰ→固_(Ⅱ)。前者的相变温度、相变焓和相变熵分别为330.6±0.1K,47.78±0.29kJ·mol~(-1)和144.5±0.9J·K~(-1)·mol~(-1),后者的对应相变热参数分别为334.5±0.1K,5.96±0.05kJ·mol~(-1)和17.82±0.15J·K~(-1)·mol~(-1)。报道了该物质每隔10K的热力学性质.     

四氯合金属(Ⅱ)酸正烷铵在280—500K间的热力学性质和相变Ⅱ.四氯合锌(Ⅱ)酸正十二烷铵

在利用相变焓储存太阳能等低温热能的研究中,人们已发现无机水合盐类物质有凝析、过冷以及熔化后液体易漏出等缺点.解决这些问题的途径之一是开发固-固相变低温储能材料.(RNH_3)_2MX_4(R=长链正烷基,M=Mn,Cu,Co,Ni,Fe和Zn等二价金属,X=Cl或Br)在300—380K间有相变焓很大的固-固相变,是很有开发前景的固-固相变低温储能材料.我们在第Ⅰ报中报道过(n-C_(12)H_(25)NH_3)_2MnCl_4的绝热量热学研究结果,本文将报道(n-C_(12)H_(25)NH_3)_2ZnCl_4(1)在280—500K间的热力学性质和相变热参数.     

四氯合锌酸二(正十一烷基铵)晶体相变的Raman光谱

用Raman光谱研究了[n-C_(11)H_(23)NH_3]_2ZnCl_4(简记为C_nZn)配合物的固-固相变.结果表明,配合物产生的固-固相变主要与烷烃链的堆积结构和分子构象变化有关.在 T_(c1)=25℃的相变是由于烷烃链的侧向堆积和分子构象的有序到部分无序变化.在中间相,分子链局部产生旁式构象.在T_(c2)=87℃的相变主要来源于烷烃链从部分构象有序到完全无序的变化.高温相形成了构象完全无序相.相应于烷烃链的“熔化”.     

新型"分子合金"类Fe(II)配合物的合成和自旋转换性能

合成了Fe[(Htrz)~9~/~4(NH~2trz)~3~/~4](BF~4)~2.H~2O(1)和Fe[(Htrz)~3~/~2(NH~2trz)](BF~4).3H~2O(2)两个"分子合金"类自旋转换配合物。其变温光谱表明,它们在室温附近具有自旋转换行为,同时还伴有热致变色及滞后现象。     

新型"分子合金"类Fe(II)配合物的合成和自旋转换性能

合成了Fe[(Htrz)~9~/~4(NH~2trz)~3~/~4](BF~4)~2.H~2O(1)和Fe[(Htrz)~3~/~2(NH~2trz)](BF~4).3H~2O(2)两个"分子合金"类自旋转换配合物。其变温光谱表明,它们在室温附近具有自旋转换行为,同时还伴有热致变色及滞后现象。     

四氯合锌酸十六烷基铵-四氯合锌酸十八烷基铵二元体系亚固相相图

合成了具有层状结构的热致相变材料四氯合锌酸十六铵(n-C16H33NH3)2ZnCl4,C16Zn)和四氯合锌酸十八铵(n-C18H37NH3)2ZnCl4,C18Zn)(在340~370 K的温度范围内存在着焓值较大的可逆固-固相变)。 并将此2种材料在乙醇溶液中结晶出一系列二元体系。 对二元体系利用差热分析(DTA)和X射线衍射技术进行测定,构筑了C16ZnC18Zn二元体系亚固相相图。 根据相图,确定了w(C16Zn)=41.11%处有中间化合物(n-C16H33NH3)(n-C18H37NH3)ZnCl4的存在,并测定在w(C16Zn)=16.19%和w(C16Zn)=63.07% 2处存在着2个不变的共析点,2个共析点温度分别约为356和353 K。 与同类体系的其它相图相比,在此相图的左右边界存在端际固溶体（α和β）和中间区域存在非化学计量相（γ）。     

RAMAN STUDIES OF STRUCTURAL PHASE TRANSITION IN[n-C_(11)H_(28)NH_8]_2ZnCl_4

The perovskite type of compound [n-C_(11)H_(23)N_3]_2ZnCl_4(abr.C_(11)Zn)exhibits two solid-solid phasetransitions at T_(c1)=298.7 K and T_(c2)=360.1 K.A temperature dependence study of Raman spectra of C_(11)Znprovides the evidence of occurence of the structural phase transition related to the dynamics of thealkylammonium ions.The room temperature phase is ordered and contains the all-trans alkyl chains.Theintermediate temperature phase presents a partial conformational disorder and liquidlike state of allconformational disorder occurs at high-temperature phase.     

四氯合铜酸二烷基铵相变的热分析和红外光谱

用DSC和TG研究了(n-C_nH_(2n+1)NH_3)_2CuCl_4(n=7-12)(记为C_nM)配合物的热稳定性和固-固相变。由红外光谱讨论了C_9Cu三个相的性质。发现C_nM的热稳定性呈奇偶效应; 主相变峰温随链长增长而升高; 相变总ΔH和ΔS也随链增长而加大; 当n≤9时, 高温相为部分无序相; 而n≤10时, 高温相为构象无序相。C_9Cu的主相变主要源自链间堆积结构变化。而在307.7 K的相变主要与烃链有序-无序变化有关。     

Phase Transitions in Crystalline [M(H2O)6](ClO4)2 (M=Mg,Mn, Fe,Co, Ni,Cu, Zn,Cd and Hg)

The results of DSC measurements in the temperature range 140–370 K on nine crystalline compounds of the type [M(H₂O)₆](ClO₄)₂, where M=Mg, Mn, Fe, Co, Ni, Cu, Zn, Cd and Hg, are discussed. Anomalies detected in the DSC curves are related to the existence of solid-solid phase transitions and/or to the melting points of these compounds. In consequence of two different hypothetical structural modifications of [Fe(H₂O)₆](ClO₄)₂, two DSC curves are obtained. For the compounds with M=Fe, Cd and Hg, new phase transitions have been discovered. The transition temperatures of the other phase transitions are in good agreement with literature data obtained by adiabatic calorimetry. For the compounds with M=Mg, Ni and Cd, DTA measurements were also carried out and the melting points of theses compounds were established. This revised version was published online in August 2006 with corrections to the Cover Date.     

(n-C18H37NH3)2MCl4热容的测定

在差示扫描量热仪(DSC仪)上, 采用扫描热焓法测定物质的热容, 实验精度达到±1%左右. 在190-410 K温度区间内, 测定了四氯合金属酸(Ⅱ)正十八铵(n-C_(18)H_(37)NH_3)_2MCl_4(M=Mn和Zn; 简称C_(18)M)的热容. 同时测定了C_(18)M的固-固相变焓和相变熵. 本文报导了C_(18)M每隔5 K的热力学函数.     

Metal-dependent thermal behaviour Ln (n-CnH2n+1NH3)2MCl4

Compounds of the type (n-C_nH_2n+1NH₃)₂MCl₄ with n = 12 or n = 16 and with M = Mn, Cu, Co, Fe, Hg, Zn show order-disorder solid-solid phase transitions in the temperature range 300–380 K. Three general types of thermal behaviour can be observed for compounds with different metals, but with the same n. The different thermal behaviour appears to be related to different coordination geometries at the metal atoms.     

Analysis of phase transition pathways in X3H(SO4)2 (X=Rb, NH4, K, Na): variable temperature single-crystal X-ray diffraction studies

Evaluation of phase transitions in a series of hydrogen sulfates (Rb3H(SO4)2, (NH4)3H(SO4)2, K3 H(SO4)2, and Na3H(SO4)2) based on the single-crystal structure analysis has revealed the exact nature of such transitions and has sorted out the various ambiguities involved in earlier literature. Rb3H(SO4)2 at 293 K is C2/c. It is isostructural to its ammonium analogue, (NH4)3H(SO4)2, at room temperature. However, the variable temperature single-crystal diffraction studies indicate that the phase transition mechanism is different. When cooled to 100 K, the structure of Rb3H(SO4)2 remains C2/c. When heated to 350 K, it transforms to C2/m (with double the volume at room temperature), which changes to C2/c (with 4 times the volume at room temperature) at 425 K. The high-temperature (420 K) structural phase transition in (NH4)3H(SO4)2 is shown to be Rm. The structure of Na3H(SO4)2 remains invariant (P21/c) throughout the range of 100-500 K except for the usual contraction of the unit cell at 100 K and expansion at 500 K. The structural phase transitions with temperature for the compound K3H(SO4)2 are very different from those claimed in earlier literature. The hydrogen atom participating in the crucial hydrogen bond joining the two sulfate tetrahedra controls the structural phase transitions at low temperatures in all four compounds. The distortion of the SO4 tetrahedra and the coordination around the metal atom sites control the phase evolution in the Rb compound, while the Na and K analogues show no phase transitions at high temperature, and the NH4 system transforms to a higher symmetry space group resulting in a disorder of the sulfate moiety.     

Coexistence of magnetic and electric orderings in the metal-formate frameworks of [NH4][M(HCOO)3

A family of three-dimensional chiral metal-formate frameworks of [NH(4)][M(HCOO)(3)] (M = Mn, Fe, Co, Ni, and Zn) displays paraelectric to ferroelectric phase transitions between 191 and 254 K, triggered by disorder-order transitions of NH(4)(+) cations and their displacement within the framework channels, combined with spin-canted antiferromagnetic ordering within 8-30 K for the magnetic members, providing a new class of metal-organic frameworks showing the coexistence of magnetic and electric orderings.