“二组分简单共熔体系相图测量”实验的绿色化探索

基于绿色化学理念,探索选用无毒、低熔点的“正十八醇-月桂酸”近室温有机共熔体系,通过测量步冷曲线,获取不同配比条件下体系的固液相变温度,从而绘制相图;再用差示扫描量热法对固液相变温度加以验证,显示2种方法测得的固液相变温度相互吻合,表明该二元共熔体系用于固液相图绘制实验的可行性。由于高级脂肪酸-脂肪醇体系固液相变的潜热较大,该类体系展现出有望作为潜热储能材料的应用前景。因此,该二元有机共熔体系相图测量实验,可在对实验体系进行绿色化探索的基础上,帮助学生认识相变材料和潜热储能技术。     

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     

差热分析求可逆相变焓的模拟研究

就样品的比热在相变前后均是温度函数的一般情况 ,通过动态地模拟DTA测量样品所经历的整个相变过程 ,验证了DTA中该相变潜热公式及相应的面积方法的正确性。证明对于可逆相变 ,采用文章所建议的面积法 ,把升降温过程中测得的相变潜热取一算术平均值 ,可最大限度地减少由于样品内温度梯度及样品比热是温度函数所带来的测量误差     

石蜡/十八酸/十八醇复合材料的制备及蓄/放热性能

采用石蜡、十八酸、十八醇为相变原材料,膨胀石墨作为填充式导热材料,制备了一种应用于动力电池散热的新型复合相变材料。用差示扫描量热仪(DSC)测试了热流率随温度的变化规律,其中十八酸主要影响相变材料的相变温度区间,十八醇主要影响相变潜热。相变材料最优配比为质量分数56%石蜡+16%十八酸+28%十八醇,其熔融相变温度为48℃,相变潜热为241.9 kJ/kg。在蓄/放热装置中加入含不同质量分数的膨胀石墨的相变材料,能够增加相变材料的导热性,同时会使热量的分布更加均匀,减弱了温度不均衡现象;在不同水平面上,加入膨胀石墨会导致位于下层的相变材料的加热速度更快;在同一水平面上,相变材料的加热速度与温度的传递方向一致,即加热壁面在外,则传热方向由外向内,加热速度由外至内呈逐渐减缓。     

差热分析的相转变终点和相转变焓Speil公式的理论分析

本文通过考虑容器和试样内存在温度梯度这一事实,成功地解释了实际DTA曲线上的相变终点,并就相变前后试样的热容量不同这一普遍情况,推导出计算热焓的广义Speil公式。     

新型低温复合相变蓄冷材料的研制

根据凝固点降低理论自行研制出一种-10℃以下的低温相变材料。首先将筛选得到的有机醇、无机盐和水按照一定比例配制出低温相变材料,利用步冷曲线法找到合适的共晶点,利用DSC测试法得到其相变潜热,瞬态平面热源法得到热导率。最终得到相变温度为-14.8℃、相变潜热225.9 kJ/kg、导热率为0.57 W/(m·K)的低温相变材料。     

DSC曲线各特征点的物理意义以及相变热焓的广义Speil公式的推导

按目前差示扫描量热法（DSC）公认的Gray－Speil理论，由于对实际的过程过于简化，以致不能很好地解释DSC曲线上的每个特征点；就相变前后试样的热容量发生改变的普遍情况下，如何定量计算相变潜热，目前尚未有严格的计算理论。本文对差示扫描量热法的基本理论做了一些较深入的探索，通过考虑容器及试样内存在温度梯度这一实际情况，成功地解释了实际DSC曲线上各个特征点具体的物理意义，并就相变前后试样的热容量发生变化且热容量是温度的函数这一普遍情况，推广出广义的Speil公式和热焓计算的普遍法则，得到了与实验更加接近的结果。     

细粒径石蜡微胶囊相变材料的制备与性能

采用阳离子和非离子复配乳化剂,通过原位聚合制备以丙烯酸酯为壁材,石蜡为芯材的细粒径微胶囊相变材料.采用傅里叶变换红外光谱(FTIR)、扫描电子显微镜(SEM)、差示扫描量热(DSC)、热重(TG)及激光粒度仪分析表征了微胶囊相变材料的化学结构、表面形貌和热性能.结果表明,乳化剂的种类和壁材单体的配比对微胶囊性能有重要的影响.当采用阳离子和非离子复配乳化剂,壁材中单体甲基丙烯酸甲酯(MMA)与丙烯酸(AA)的质量比为9∶1时,微胶囊相变材料呈球形且表面光滑紧凑,尺寸仅为0.2~0.35μm,具有良好的储热能力,相变潜热高达169 J/g;微胶囊中壁材对石蜡芯材的分解具有明显热阻滞作用,分解温度比纯石蜡提高了150℃.     

癸酸-十四烷酸二元体系的相变性能

以癸酸(CA)-十四烷酸(MA)二元体系的理论预测相图为指导, 测量了该体系不同组成超声波混合后的步冷曲线, 绘制了该体系的实验相图, 判断出最低共熔温度与组成范围; 采用DSC测试最低共熔组成的相变性能, 采用IR检测最低共熔组成300次热循环前后的波形变化. 实验结果表明, CA-MA二元体系最低共熔组成范围为(76%~82%)CA+(24%~18%)MA, 最低共熔温度为294.45 K, 最大过冷度为274.75 K, 相变过程中无分层现象; DSC和IR的测试结果表明, 组成为78%CA+22%MA的相变焓为149.02 J/g, 开始相变温度为292.80 K, 热稳定性好.     

油井用相变微胶囊的制备与性能

针对深水固井作业过程中水泥水化放热较大,易致使环空地层天然气水合物分解的技术难题,本文以石蜡为芯材,碳酸钡为壁材,制备了一种油井用相变微胶囊。首先,利用FT-IR、DSC、TGA与SEM对相变微胶囊的化学组成、热性能与微观形貌进行了表征。结果表明：相变微胶囊的封装效率为67.40%,具有较高的封装效率和良好的潜热储存能力。其次,对粒径分布与润湿性能进行了测试。结果表明：微胶囊颗粒平均粒径为4.946 μm,小于水泥颗粒粒径17.201 μm,可较好的镶嵌在水泥石中,并充填于水泥水化产物之间,减小对水泥石力学性能的负面影响;微胶囊与水的静态接触角为46.8°,具有良好的亲水性能,可应用于水基的水泥浆环境中。最后,将微胶囊应用于水泥浆体系,研究了水泥浆的水化温升和水化热。结果表明：与空白水泥浆相比,加入12%相变微胶囊水泥浆的最高水化温升与水化热（48 h）分别下降了14.56%和43.23%。      

Modulated temperature DSC measurements relating to the cold crystallization process of poly(ethylene terephtalate)

The modulated temperature differential scanning calorimetric method (MT-DSC) yields three temperature dependent signals, an underlying heat capacity curve from the underlying heat flow rate (corresponding to the conventional DSC signal), and a complex heat capacity curve with a real part (storage heat capacity) and an imaginary part (loss heat capacity). These curves have been measured in the cold crystallization region for poly(ethylene terephtalate) with a modified Perkin-Elmer DSC-7. The underlying curve shows the well known large exothermic crystallization peak. The storage heat capacity shows a step change which reproduces the change in heat capacity during crystallization. This curve may be used as baseline, to separate the crystallization heat flow rate from the underlying heat flow rate curve. The loss heat capacity curve exhibits a small exothermic peak at the temperature of the step change of the storage curve. It could be caused by changes of the molecular mobility during crystallization.Dedicated to Professor Wunderlich on the occasion of his 65th birthday     

不同实验条件对DSC峰形的影响以及相变温度的确定

本文通过深入分析实际的ＤＳＣ过程，阐述了ＤＳＣ曲线上各个特征点以及这些点所对应的物理意义。在理论上分析各种不同的实验条件对ＤＳＣ曲线形状的影响，指出目前在ＤＳＣ分析中所用的确定试样熔点的方法以及用高纯金属ＤＳＣ变曲线上熔融峰峰前沿的斜率修正试样相变温度所存在的问题，指出ＤＳＣ相变曲线刚开始偏离基线的那点所相应试样盒的温度即为试样的熔点，本文还提出了通过提高试样，试样盒以及试样支座之间的热导率，来提     

A Novel Single-pan Scanning Calorimeter. Measurement of thermophysical properties of metallic alloys

In this paper problems associated with a conventional heat-flux DSC are discussed. A single pan calorimeter has been designed and built which eliminates many of the errors that occur in a conventional DSC. It was found that: enthalpy changes and heat capacity were repeatable to better than1%; the apparent latent heat and heat capacity did not depend on specimen size or significantly on rate of heating as often occurs in a two-pan heat-flux DSC; during the melting of pure Al, more than 80% of the latent heat was evolved over a temperature of 0.04 K; in alloys, separate heat capacity peaks for different reaction less than 1 K apart were resolved. This revised version was published online in July 2006 with corrections to the Cover Date.     

Selective Water Sorbents for Multiple Applications, 10. Energy Storage Ability

The application of new selective water sorbents for storage of low temperature heat is analyzed. Values of energy storage ability E are measured by a DSC technique for more than fifteen samples of selective water sorbents based on silica gels, aluminas, carbon Sibunit and aerogels as host matrices and CaCl₂, LiBr, MgCl₂ as impregnated salts. E-values up to 8.4 kJ/g and 4.0 kJ/g are found for forced and naturally saturated sorbents, which are much higher than for common sorbents, like zeolites and unimpregnated silica gels. The temperature dependence of E gives an estimation of sensible and latent heat contributions as well as the average heat of water desorption and average specific heat of dry sorbents. A comparison between the SWSs and others materials proposed in literature is done.     

Reversible and irreversible heat capacity of poly[carbonyl(ethylene‐co‐propylene)] by temperature‐modulated calorimetry

The heat capacity of poly[carbonyl(ethylene‐co‐propylene)] with 95 mol % C₂H₄? CO? (Carilon EP®) was measured with standard differential scanning calorimetry (DSC) and temperature‐modulated DSC (TMDSC). The integral functions of enthalpy, entropy, and free enthalpy were derived. With quasi‐isothermal TMDSC, the apparent reversing heat capacity was determined from 220 to 570 K, including the glass‐ and melting‐transition regions. The vibrational heat capacity of the solid and the heat capacity of the liquid served as baselines for the quantitative analysis. A small amount of apparent reversing latent heat was found in the melting range, just as for other polymers similarly analyzed. With an analysis of the heat‐flow rates in the time domain, information was collected about latent heat contributions due to annealing, melting, and crystallization. The latent heat decreased with time to an even smaller but truly reversible latent heat contribution. The main melting was fully irreversible. All contributions are discussed in the framework of a suggested scheme of six physical contributions to the apparent heat capacity. © 2001 John Wiley & Sons, Inc. J Polym Sci Part B: Polym Phys 39: 1565–1577, 2001     

Can one measure precise heat capacities with DSC or TMDSC?</o:p>

Summary During a prior study of gel-spun fibers of ultrahigh-molar-mass polyethylene, a substantial error was observed on calculating the heat capacity with a deformed pan, caused by the lateral expansion of the fibers on shrinking during fusion. In this paper, the causes of this and other effects that limit the precision of heat capacity measurements by DSC and TMDSC are explored. It is shown that the major cause of error in the DSC is not a change in thermal resistance due to the limited contact of the fibers with the pan or the deformed pan with the platform, but a change in the baseline. In TMDSC, the frequency-dependence is changed. Since irreversible changes in the baseline can occur also for other reasons, inspections of the pan after the measurement are necessary for precision measurements.     

Real-time image analysis and numerical simulation of isothermal spherulite nucleation and growth in polyoxymethylene

A method of analysing nucleation and crystallization kinetics, based on real time image analysis and hot stage optical microscopy, has been used to investigate the isothermal crystallization of different grades polyoxymethylene. The data were compared with results from differential scanning calorimetry (DSC), using a simple numerical simulation to model the effects of finite smaple thickness on the form of the isothermal DSC curves. This simulation was then used to predict the microstructural development in a bulk sample for different boundary conditions, taking into account latent heat evolution and diffusion during crystallization.     

Heat capacity of cheese

The heat capacity of several samples of hard cheese, semi-hard cheese and soft cheese was determined by conventional differential scanning calorimetry (DSC) and by temperature modulated DSC. Additionally, the gross composition of the cheeses was analysed, and equations from the literature were used to calculate the heat capacity therefrom. Both analytical methods were suitable to determine the heat capacity of the cheese samples whereas only one out of three equations proposed for the calculation of the heat capacity of foods from composition data led to results which were comparable with analytical data. As the equation coefficients for particular constituents are responsible for the deviations in the calculated heat capacities the differences between calculated and measured values increase with a decreasing moisture content of the cheeses.     

Thermodynamic properties and thermal stability of the synthetic zinc formate dihydrate

Zinc formate dihydrate has been synthesized and characterized by powder X-ray diffraction, elemental analysis, FTIR spectra and thermal analysis. The molar heat capacity of the coordination compound was measured by a temperature modulated differential scanning calorimetry (TMDSC) over the temperature range from 200 to 330 K for the first time. The thermodynamic parameters such as entropy and enthalpy vs. 298.15 K based on the above molar heat capacity were calculated. The thermal decomposition characteristics of this compound were investigated by thermogravimetric analysis (TG) and differential scanning calorimetry (DSC). TG curve showed that the thermal decomposition occurred in two stages. The first step was the dehydration process of the coordination compound, and the second step corresponded to the decomposition of the anhydrous zinc formate. The apparent activation energy of the dehydration step of the compound was calculated by the Kissinger method using experimental data of TG analysis. There are three sharply endothermic peaks in the temperature range from 300 to 650 K in DSC curve.     

Estimation of Ethyl Cellulose Layer Thickness of Coated Polyethylene Oxide Particles Using Differential Scanning Calorimetry

Particles of poly(ethylene oxide) (PEO) were coated using ethyl cellulose (EC). Equations and a method were proposed to estimate the EC layer thickness by using differential scanning calorimetry (DSC) based on melting or crystallization heat of phase-change materials. The result shows that EC layer thickness of polyethylene oxide particles determined using DSC is consistent with the result using an optical microscope.