无水磷脂DHPC的相变及水含量影响的DSC研究

利用差示扫描量热法,研究了无水及含水的1,2-双正十七烷酰基磷脂酞胆碱(DHPC)的相变特性.实验发现,无水DHPC初次受热时,首先发生玻璃态转变,接着像通常的晶体一样熔化.因此是玻璃性晶体.从熔体中结晶的DHPC是通常的晶体.从可以冻结水的总熔化培Q_f和水含量h的关系断定:在含水DHPC中,水可以存在于3种热力学上可区分的状态.第1种是不可冻结水,它是与磷脂头基直接结合的水,是一级水合水.每个头基最多可结合7个这样的水分子.第2种是二级水合水,其熔点接近于纯水但其比熔比焓dQ_f/dh比纯水的低.每个DHPC分子最多可保有约6个这样的水分子.当h再增大时,体系中有熔点及比熔化焓接近于纯水的体相水.实验发现,h增加,DHPC熔化峰向低温方向移动;当h>16.2%时,其凝胶-液晶相变温度T_tr及相交焓面△H_tr基本上不随h变化.T_tr、△H_tr及相变熵△S_(tr)的实验值和从偶数碳酰基磷脂酰胆碱同系物中得到的Huang(1981)方程组的计算值吻合.     

过量水中脑磷脂假二元系相变的DSC研究

运用差示扫描量热法研究了过量水中脑磷脂 (DMPE和DHPE)假二元系的凝胶 液晶相变 ,给出该假二元系的相图 .实验表明 ,至少在DHPE的摩尔分数低于0 1时可能出现部分相分离现象 .理想溶液模型分析表明 ,既在凝胶相 ,又在液晶相 ,这两个脑磷脂都不理想混溶 ;正规溶液模型分析表明 ,凝胶相的非理想性参数更大     

磷脂DHPC和短杆菌肽D相互作用的DSC研究

Changes of the behavior of the thermotropic phase transitions of the phospholipid DHPC by the action of miniprotein gramicidin D (G.D) have been studied by differential scanning calorimetry. The experimental results demonstrated that G.D could not remove the pretransition of DHPC, but the pretransition peak and the main transition peak of DHPC were incorporated into a broad peak. The pretransition temperature and the main transition temperature of DHPC decreased to different ex-tent. The sums of the pretransition and main transition enthalpies of DHPC showed a lineally decreasing relationship with increasing the mole fraction x_g of gramicidin D.     

稀土离子及其配合物对二棕榈酰磷脂酰乙醇胺相变性质的影响

用差示扫描量热研究了金属离子和稀土配合物对二棕榈酰磷脂酰乙醇胺(DPPE)脂双层由凝胶态向液晶态相转变的影响T~m的影响。发现加入金属离子提高了DPPE脂双层的相转变温度。其中, Na^+＜Ca^2^+＜Ln^3^+。Pr^3^+的影响较La^3^+强。在pH 7.4时, 柠檬酸镧对T~m影响很小, 相反在pH 2.0时, 则降低相变温度T~m。乳酸稀土在pH 2.0和pH 7.4时都显著提高T~m, 在中性条件下, 对T~m影响更大。同时, 乳酸稀土较相同浓度下的稀土离子影响大, 说明乳酸稀土中稀土离子和乳酸根配体存在协同作用。我们初步探讨了金属离子以及稀土配合物对DPPE脂双层相变温度影响的原因。     

磷脂酰胆碱相变热力学参数的同系线性规律性

两亲性磷脂是生物膜的主要成分，以双分子层结构存在干股中．当脂质双分子层中含足够比例的液晶相时，膜才有一定的流动性，细胞才能生长繁殖．因此，生物膜脂质双分子展相变特别是凝胶一液晶棺变研究历来为学界所重视．在正烷烃中，人们已观察到从。相到转子相（rotomericPhas     

差示扫描量热法中相变潜热公式的推导

通过考虑热分析过程中存在于试样内的温度梯度,就相变前后试样的比热容发生变化、并且是温度的函数这一普遍情况,推导得到了普遍的用差示扫描量热法求相变潜热的公式     

水合和pH对蛋白酶K热诱发转变影响的量热法研究

用差示扫描量热法, 在310～450 K温度范围、0.048～4.39克水/克干酶以及pH3～9范围内研究了蛋白酶K(EC 3.4.21.14)的热变性。分别提出表征热变性过程的三个主要热力学参数: 热变性温度T_d、比变性焓△H_d及超额表观比热C_(ex)~(max)和总水量h以及pH的关系。除Td和h的关系属于Flory-Garrett类型外, 蛋白酶K的热变性热力学特征和已报道的球蛋白、双螺旋蛋白及三螺旋蛋白不相同。一级水合水对蛋白酶K热变性热力学特征有最大的影响, pH也是影响该酶热稳定性的重要因素。     

大分子拥挤环境中脂肪酸影响磷脂囊泡相变的差示扫描量热研究

脂肪酸诱导的磷脂膜的热力学行为对于认识细胞内复杂的机制有着重要意义,而前人在研究脂肪酸与磷脂膜相互作用时大都在稀溶液中进行;拥挤环境下脂肪酸诱导磷脂膜的相变行为还未见报道。本文以二肉豆蔻酰磷脂酰胆碱(DMPC)构建囊泡模型,采用差示扫描量热法系统地研究了在不同浓度、不同分子量的聚乙二醇(PEG)拥挤环境中不同结构的脂肪酸对DMPC磷脂囊泡相变的影响。研究结果表明,在拥挤环境中,PEG对纯的磷脂囊泡相变的影响与大分子的分子量和浓度相关。对于脂肪酸/磷脂囊泡(FA/DMPC),PEG的存在对囊泡相变产生显著影响。在所考察的分子量和浓度范围内,PEG使FA/DMPC囊泡相变增加。短链饱和脂肪酸、不饱和脂肪酸原本使DPMC囊泡相变降低,但PEG缩小了降低幅度,甚至导致相变增加。进一步的研究表明,在大多数情况下,PEG对FA/DMPC的相变具有协作增强效应,且其影响均与大分子的分子量和浓度相关。另外,随着PEG浓度的升高,磷脂囊泡的协同单位数逐渐降低,表明拥挤环境会影响磷脂双分子层的均一性,使协同发生相变的分子数降低。本文的研究表明,大分子拥挤环境能够对扰动的磷脂双分子层起到一定的修复作用,这一现象在生物膜相关领域不可忽视。     

示差扫描量热法进展及其在高分子表征中的应用

示差扫描量热法(DSC)是表征材料热性能和热反应的一种高效研究工具,具有操作简便、应用广泛、测量值物理意义明确等优点.近年来DSC技术的发展大大拓展了高分子材料表征的测试范围,促进了对高分子物理转变的热力学和动力学的深入研究.温度调制示差扫描量热法(TMDSC)是DSC在20世纪90年代的标志性进展,它在传统DSC的线性升温速率的基础之上引入了调制速率,从而可将总热流信号分解为可逆信号和不可逆信号两部分,并能测量准等温过程的可逆热容.闪速示差扫描量热法(FSC)是DSC技术近年来的创新性发展,它采用体积微小的氮化硅薄膜芯片传感器替代传统DSC的坩埚作为试样容器和控温系统,实现了超快速的升降温扫描速率以及微米尺度上的样品测试,使得对于高分子在扫描过程中的结构重组机制的分析以及对实际的生产加工条件的直接模拟成为可能.本文从热分析基础出发,依次对传统DSC、TMDSC和FSC进行了介绍,内容覆盖其发展历史、方法原理、操作技巧及其在高分子表征中的应用举例,最后对DSC未来的发展和应用进行了展望.本文希望通过综述DSC原理、实验技巧和应用进展,帮助读者加深对DSC这一常用表征技术的理解,进一步拓展DSC表征高分子材料的应用.     

DSC测量中校正对热分析结果的影响

介绍了灵敏度及温度校正对基线和实验结果的影响.仪器温度和灵敏度校正可以减小差示扫描量热法(DSC)曲线的漂移,曲线上得到的温度和焓变值更接近理论值,减小了实验误差.所以,定期对仪器进行重新校正是必要的.     

Synthesis,Structural Study and Phase Transitions Characterization by Thermal Analysis and Vibrational Spectroscopy of an Ammonium Rubidium Arsenate Tellurate

The Rb_2.42(NH₄)_0.58(HAsO₄)(H₂AsO4)·Te(OH)₆ crystals(denoted by RbNAsTe) crystallize in the monoclinic system, space group P2₁/n with the following parameters:a=1.3059(5) nm, b=0.6755(3) nm, c=1.6675(6) nm, β=94.126(4)°, Z=4 and V=1.46733(10) nm³. Thermal analyses(DSC, DTA and TG) confirm the presence of the phase transition and the temperature of the decomposition. The vibrational spectroscopy study at room temperature show the presence and the independence of anionic groups, cationic groups, and give more importance to the hydrogen bonds. Raman spectra were recorded in the temperature range of 298-503 K. The temperature dependence of the Raman line shift, intensity reduction and the half width detects the phase transitions and confirms their nature. So, the phase transition at 453 K corresponds to the superprotonic-ionic conduction phase transition, and those at 483 and 491 K correspond to the decomposition of our material.     

Experimental Investigation on Binary Phase Diagram of the Thermotropic Phase Transitions Compounds (n‐CnH2n+1R3)2ZnCl4

The thermotropic phase transitions compounds (n‐C_nH_2n+1R₃)₂ZnCl₄ as well as a series of their binary mixtures were prepared by a solution reflux method from their ethanol solutions. The experimental subsolidus binary phase diagram of [n‐C₁₈H₃₇N(CH₃)₃]₂ZnCl₄‐[n‐(C₁₈H₃₇)₂N(CH₃)₂]₂ZnCl₄ is constructed over the entire composition range by differential scanning calorimetry(DSC) and X‐ray. Experi‐ mental results indicate one stable intermediate phase [n‐C₁₈H₃₇N(CH₃)₃] [n‐(C₁₈H₃₇)₂N(CH₃)₂]ZnCl₄ at W_C18C3Zn %=59.75 %, and two invariant three phase equilibria, which shows two eutectoid temperatures: Te₁ at 310±1 K for eutectoid point W_C18C3Zn %=36.24 %, Te₂ at 313±1 K for eutectoid point W_C18C3Zn %=80.17 %. These three noticeable solid‐solution ranges are α‐phase at the left, ?‐phase at the right, and ψ‐phase in the middle of the phase diagram. It is (n‐C_nH_2n+1R₃)₂ZnCl₄ systems as phase change materials that are characterized the phase transition temperatures T in the range of 310 to 340 K, the transition enthalpies ΔH in the range of 38.40 and 168.72 J/g between two polymorphic forms.     

Specific heat studies in a-Se and a-Se<Subscript>90</Subscript>M<Subscript>10</Subscript> (M = In,Sb, Te) alloys

Specific heat measurements have been made in a-Se and a-Se₉₀M₁₀ (M = In, Sb, Te) alloys using differential scanning calorimetry (DSC) technique to see the effect of additives In, Sb and Te on the specific heat in a-Se. An extremely large increase in the specific heat values has been observed at the glass transition temperature. It has also been found that the values of C _p below glass transition temperature (C _pg ) and after glass transition (C _pe ) are highly composition dependent. This indicates that the additives used in the present study influences the structure of the a-Se. Specific heat and atomic mass values of the additive elements are found to be significant for the explanation of present results.     

Two novel phase transition materials based on 1-isopropyl-1,4-diazabicyclo[2.2.2]octan-1-ium

Two novel phase transition materials,[C₉H₂₀N₂] [Na(BF₄)₃] (1) and[C₉H₂₀N₂] [(PF₆)₂] (2), were synthesized based on 1-isopropyl-1,4-diazabicyclo[2.2.2]octan-1-ium with sodium tetrafluoroborate and hexafluorophosphoric acid, respectively. Differential scanning calorimetry measurements detected that 1 and 2 underwent reversible phase transitions, which were confirmed by dielectric measurements. Single crystal X-ray diffraction data suggested that compound 1 changed from a high temperature phase with a space group of P6₃ to a low temperature one with a space group of P2₁/c, and that compound 2 transformed from the space group of Pbca at room temperature to P2₁/c at low temperature. Formation of hydrogen bonds and distortion of 1,4-diazabicyclo[2.2.2]octane rings may drive the transitions.     

Phase transition of aqueous solutions of poly(N,N-diethylacrylamide-co-acrylic acid) by differential scanning calorimetric and spectrophotometric methods

 The phase transition of aqueous solutions of poly(N,N-diethylacrylamide-co-acrylic acid) (DEAAm–AA) is studied by differential scanning calorimetry (DSC) and UV–vis spectrophotometry. The copolymer aqueous solutions are shown to have well-defined lower critical solution temperatures (LCSTs). The LCST values obtained from the maximum of the first derivatives of the DSC and optical transition curves agree well. DSC can be used to measure the phase-transition temperature of more dilute polymer solutions. On increasing the AA composition in the copolymers, the LCST values of the copolymer increase, then decrease at higher AA composition. For the aqueous solution of the copolymers, the transition curve obtained by the spectrophotometric method is highly wavelength dependent. The LCST values are found to be concentration-dependent. The changes in the heat of the phase transition of the copolymer solutions measured from DSC are lower than that of the homopolymer PDEAAm solution. This is consistent with the suggestion that the polymer chains of the copolymers collapsed only partially at temperatures above the LCST. The added salt (sodium chloride) decreases the transition temperature of the polymer solution. Received: 14 November 2000 Accepted: 15 January 2001     

Effects of moisture on glass transition and microstructure of glycerol-plasticized soy protein

The glass transition behavior of the glycerol-plasticized soy protein sheets (SL series) at various relative humidity (RH) was investigated by using differential scanning calorimetry with the aluminum pan and O-ring-sealed stainless steel capsule, and the microstructure of these sheets was detected on small-angle X-ray scattering. The results revealed that there were three glass transitions (Tg1, Tg2 and Tg3), corresponding to glycerol-rich, protein-rich and protein-water domains, in the protein-glycerol-water ternary system. The Tg1 values of the SL-series sheets at 75% RH decreased from -49.3 to -83.8 degrees C with an increase of glycerol content from 10 to 50 wt.-%, whereas Tg2 and Tg3 were almost invariable at about 60 degrees C and 3 degrees C, respectively. In addition, the Tg1, Tg2 and Tg3 values of the SL-25 containing 25 wt.-% glycerol at 0%, 35%, 58%, 75% and 98% RH were in the range of -12.7 - -83.2 degrees C, 65.8 - 53.1 degrees C and 3.5 - 1.9 degrees C, respectively. The result from small-angle X-ray scattering indicated that the radii of gyration (Rg) of protein-rich domain were in the range of 60-63 nm; this suggested the existence of protein macromolecules as aggregates in the stable protein-rich and protein-water domains. With an increase of RH, the tensile strength and Tg values of the SL-series sheets decreased, but the elongation at break increased. In view of the results above, the moisture in ambient environment significantly influenced the Tg values and microstructures of the glycerol-plasticized soy protein sheets, leading to the changes of the mechanical and thermal properties.     

Experimental Binary Phase Diagram of Bilayer Compounds [n-CnH2n+1N(CH3)3]2CoCl4

Compounds [n-C_nH_2n+1N(CH₃)₃]₂CoCl₄(n=16, C₁₆C₃Co; n=18, C₁₈C₃Co) containing lipid-like bilayers embedded in a crystalline matrix exist in solid-solid phase transition. The low-temperature bilayer structures of the two compounds were organized by neutralizing CoCl₄^2- with alkylammonium ions. Alkyl chains lay parallel to each other and slightly tilted with respect to the normal of the inorganic layers. The adjacent alkyl chains interacted with each other by van der Waals interaction. When the temperature increased, the two compounds underwent a reversible solid-solid phase transformation within 310―330 K. In such a case, the chains showed a large motional freedom, and a disordered phase appeared. The structures can alternatively be viewed as a double layer of alkylammonium ions between CoCl₄^2- sheets and be considered as crystalline models of lipid bilayers. The experimental subsolidus binary phase diagram of [n-C₁₆H₃₃N(CH₃)₃]₂CoCl₄-[n-C₁₈H₃₇N(CH₃)₃]₂CoCl₄ was constructed over the entire composition range by differential scanning calorimetry and X-ray diffraction technique. Experimental phase diagram indicates one stable intermediate phase [n-C₁₆H₃₃N(CH₃)₃][n-C₁₈H₃₇N(CH₃)₃]CoCl₄ at w_C16C3Co= 39.89% and two invariant three- phase equilibria, which shows two eutectoid temperatures: T_e1 at (316±1) K for w_C16C3Co= 27.35% and T_e2 at (313±1) K for w_C16C3Co=59.76%. These three noticeable solid-solution ranges are α-phase at the left, β-phase at the right, and γ-phase in the middle of the phase diagram.     

端炔基对水溶液中聚(N-异丙基丙烯酰胺)相转变的影响

通过原子转移自由基聚合,制备出低分子量、窄分布、端炔基的线形聚(N-异丙基丙烯酰胺)(alkynylPNIPAM),利用高灵敏示差扫描微量热技术,在升—降温循环过程中确定端炔基对alkynyl-PNIPAM相转变行为的影响.结果显示,随循环次数增加,升温热容曲线明显变宽,降温热容曲线由双峰逐渐变为单峰;升温和降温的相转变温度有逐渐降低的趋势,但焓变的变化很小.聚合物的低的分子量使端基效应不可忽视,alkynylPNIPAM的端炔基可诱导分子链聚集,形成小的端基聚集体,由于这些聚集体中链内和链间氢键作用,链构象调整变得困难,导致PNIPAM链在升温时更易塌缩、降温时更难解离.