Sm-Fe-Si-C非晶合金的晶化动力学

用差热分析（ＤＴＡ）,结合Ｘ射线衍射（ＸＲＤ）研究了Ｓｍ－Ｆｅ－Ｓｉ－Ｃ非晶态合金的晶化动力学。结果表明：温度低于９００℃时,该合金晶化相为α－Ｆｅ（Ｓｉ）固溶体和Ｓｍ２（Ｆｅ,Ｓｉ）１７Ｃｘ。α－Ｆｅ（Ｓｉ）相的晶化表观激活能为４３１．５１ｋＪ／ｍｏｌ,Ｓｍ２（Ｆｅ,Ｓｉ）１７Ｃｘ相的晶化表观激活能为５１４．４３ｋＪ／ｍｏｌ。上在晶化初期活能变化不大,当α－Ｆｅ（Ｓｉ）相的体积分数大于７０％,Ｓ     

THE ORDERING OF THE α-Fe(Si)PHASE IN Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9 ANNEALED ALLOY

用ＸＲＤ法研究了退火Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９合金中α－Ｆｅ（Ｓｉ）晶化相的有序化过程，结果表明，Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９非晶合金在４９０℃，１ｈ退火后，α－Ｆｅ（Ｓｉ）晶化相是具有ＤＯ３结构的有序相，有序畴为球形，直径为７．０ｎｍ，它随退炎温度的升颃是长大，在５９０℃退火后达１０．９ｎｍ，与α－Ｆｅ（Ｓｉ）的尺寸相当，此时α－Ｆｅ（Ｓｉ）的有序度为０．８，在８５０℃     

Sm8Fe83Si2C5Cu0.5Nb1.5非晶合金的晶化动力学

用差热分析（ＤＴＡ）,结合Ｘ射线衍射（ＸＲＤ）研究了Ｓｍ８Ｆｅ８３Ｓｉ２Ｃ５Ｃｕ０．５Ｎｂ１．５非晶合金的晶化动力学。结果表明：温度在０￣１０００℃范围内,该合金的晶化相为α－Ｆｅ和Ｓｍ２（ＦｅＳｉ）１７Ｃｘ,α－Ｆｅ相的晶化表观激活能力３４９．５３ｋＪ／ｍｏｌ,Ｓｍ２（ＦｅＳｉ）１７Ｃｘ的晶化表观激活能力３１６．１９ｋＪ／ｍｏｌ,两相在晶化初期激活能量小,随晶化量（ｘｃ）的增加激活能增大,当α－     

退火Fe_（73．5）Cu_1Nb_3Si_（13．5）B_9合金中α－Fe（S

用ＸＲＤ法研究了退火Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９合金中α－Ｆｅ（Ｓｉ）晶化相的有序化过程．结果表明，Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９非晶合金在４９０℃，１ｈ退火后，α－Ｆｅ（Ｓｉ）晶化相是具有ＤＯ３结构的有序相，有序畴为球形，直径为７．０ｎｍ，它随退火温度的升高而长大，在５９０℃退火后达１０．９ｎｍ，与α－Ｆｅ（Ｓｉ）的尺寸相当．此时，α－Ｆｅ（Ｓｉ）的有序度为０．８在８５０℃，１ｈ退火后，α－Ｆｅ（Ｓｉ）的ＤＯ３超点阵线条消失．在５５０℃等温退火时，α－Ｆｅ（Ｓｉ）的ＤＯ３有序畴先为椭球状，于６０ｍｉｎ退火后形成球状，直径为１０ｎｍ．     

Fe73.5Cu1Nb3Si13.5B9非晶合金的晶化动力学

用ＤＴＡ结合ＸＲＤ了Ｆｅ７３．５Ｃｕ１Ｎｂ３Ｓｉ１３．５Ｂ９晶合金的晶化动力学。表明，该事金在５００℃时析出α－Ｆｅ（Ｓｉ）相。晶化初期激活能最小为２４２ｋＪ／ｍｏｌ，它随晶化量的增加，在ＸＣ为０．４－０．８时，呈极大值为５２０ｋＪ／ｍｏｌ。在６２４℃时析出Ｆｅ２Ｂ相。     

掺杂对纳米氧化铁晶化相的影响

用Ｘ射线衍射、透射电镜和穆斯堡尔谱对由掺杂了不同比例Ｓｂ的溶液－凝胶系统制得的α－Ｆｅ２Ｏ３纳米晶的晶粒度和精细结构进行了研究。结果显示，未掺杂时由Ｆｅ（ＯＨ）３非晶相干凝胶晶化而得的α－Ｆｅ２Ｏ３相晶粒较大；掺Ｓｂ后，干凝胶晶化时一部分Ｓｂ参与形成ＦｅＳｂＯ４晶相，另外的Ｓｂ原子进入α－Ｆｅ２Ｏ３晶相中形成间隙式固溶体；系统中掺杂量增多，固溶于α－Ｆｅ２Ｏ３晶相中的Ｓｂ浓度相庆也增大，它们很可能     

Fe73.5Cu1Mo3Si13.5B9非晶合金的晶化动力学

用ＤＴＡ，结合ＸＲＤ，ＴＥＭ研究了Ｆｅ７３．５Ｃｕ１Ｍｏ３Ｓｉ１３．５Ｂ９软磁非晶合金的晶化动力学，结果表明，该合金在４７８℃时析出ａ－Ｆｅ相，晶化初期激活能量最小（１４８ｋＪ．ｍｏｌ＾－１），它随晶化学量的增加而增大，在ＸＣ为５０－７８％时，呈极大值（５１０ｋＪ．ｍｏｌ＾－１）随退火温度的升高，α－Ｆｅ相的数目增多，但尺寸基本不变。为１４－１６ｍｍ。     

等温退火Fe73.5Cu1Mo3Si13.5B9合金的纳米晶结构及其与起…

本文用ＸＲＤ和ＴＥＭ研究了Ｆｅ７３．５Ｃｕ１Ｍｏ３Ｓｉ１３．５Ｂ９非晶合金在５２０℃２０－１２０ｍｉｎ退火后形成的纳米晶结构。结果表明，晶化相为局部具有ＤＯ３超结构的α－Ｆｅ（Ｓｉ），尺寸约为１４ｎｍ，α－Ｆｅ（Ｓｉ）晶粒由ＤＯ３有序区和序区组成。随退火时间的延长，α－Ｆｅ（Ｓｉ）的体积分数，Ｓｉ含量及ＤＯ３有序区尺寸增加。在退火时间为６０ｍｉｎ时，残余非晶相处于一特殊结构状态。α－Ｆｅ（Ｓｉ）相     

预退火对Fe73.5Cu1Mo3Si13.5B9纳米晶合金形成的影响

采用Ｘ射线衍射，电子衍射及透射电子显微技术研究了Ｆｅ７３．５Ｃｕ１－ｘＭｏ３Ｓｉ１３．５Ｂ９非晶合金４１０℃预退火对随后４８０℃退火所形成的纳米晶结构的影响。结果表明，预退火对Ｆｅ７３。０５，Ｃｕ１Ｍｏ３Ｓｉ１３．５Ｂ９合金纳米晶结构的形成有重要影响。当预退火时间从０小时增加到３小时，合金在４８０℃，小时退火形成的晶相化α－Ｆｅ（Ｓｉ）的晶粒尺寸从１５ｎｍ减小到８ｎｍ。预退火使α－Ｆｅ（Ｓｉ）相的     

Cu和Nb对非晶态Fe—Si—B合金等温晶化过程的影响

采用示差扫描量热卡计（ＤＳＣＩ）得到了非晶态Ｆｅ－Ｓｉ－Ｂ合金加入Ｃｕ和Ｎｂ后的等温晶化放热曲线，结合Ｘ射线衍射（ＸＲＤ）分析，明确了Ｃｕ和Ｎｂ在形成纳米α－Ｆｅ（Ｓｉ）晶体相时的作用。此外，非晶态Ｆｅ７６．５Ｓｉ１３．５Ｂ９Ｃｕ１Ｎｂ３等温化的α－Ｆｅ（Ｓｉ）放热峰呈明显的非对称形状。     

Amorphization and crystallization characteristics of TiNi shape memory alloys by severe plastic deformation

Differential scanning calorimetry (DSC) was used to determine the crystallization fraction and rate in TiNi alloys by severe plastic deformation. Results showed that the reverse martensitic transformation peak was not observed during the first heating at the rate of 40 K/min in the as-rolled samples, but one exothermic peak was observed at 620 K, which was associated with the amorphous crystallization process. During the second heating, reverse martensitic transformation was recovered. The onset crystallization temperature was low in the initial stage of crystallization with lower heating rates, but the crystallization fraction was found to increase with increasing temperature. However, the crystallization fraction was almost constant in the initial stage of crystallization with a relatively high heating rate. In all heating rates, the amorphous crystallization rates almost always reached maximum as the volumetric fraction of amorphous crystallization rose to 50%.     

蒙脱土填充聚丙烯的等温结晶动力学

用示差扫描量热法(DSC)研究蒙脱土对聚丙烯的等温结晶的影响，结果表明，蒙脱土对聚丙烯的结晶起到了异相成核的作用，提高了聚丙烯的结晶速率，结晶一半时的时间tl／2明显缩短，熔点升高，结晶度增大。用Avrami方程进行等温结晶动力学研究，参数n对结晶温度有依赖性，PP／Mont复合材料的k值随温度的升高而减小。     

聚对苯二甲酸乙二醇酯熔体等温结晶的焓松弛

利用微分扫描热分析（DSC）获得了聚对苯二甲酸乙二醇酯（PET）熔体等温结晶过程焓松弛速率曲线,并对结晶焓松弛速率曲线进行微分从而获得等温结晶焓松弛加速度曲线。文中通过定义相对结晶速率R和相对结晶加速度A,确定了相对结晶速率R和相对结晶加速度A与结晶焓松弛速率和结晶焓松弛加速度之间对应相差的一个常数值,然而其所对应的变...     

聚丙烯双模式取向结晶

利用X射线衍射仪，研究了聚丙烯熔体在应力场下双模式取向结晶的形成以及热处理、拉伸等对双模式取向结晶分布的影响。结果表明，熔体在高应力场下有利于c轴取向结晶，拉伸及热处理等影响聚丙烯双模式取向的分布。     

Effect of low multi-walled carbon nanotubes loading on the crystallization behavior of biodegradable poly(butylene adipate)

The effect of low carboxyl-functionalized multi-walled carbon nanotubes (f-MWCNTs) loading on the crystallization behavior of biodegradable poly(butylene adipate) (PBA) was studied with various techniques in this work. For the nonisothermal melt crystallization, f-MWCNTs accelerate the crystallization process of PBA apparently due to the heterogeneous nucleation effect. The Ozawa method fails to describe the nonisothermal crystallization process of neat PBA and its nanocomposite. Isothermal melt crystallization kinetics of neat PBA and its nanocomposite was analyzed by the Avrami equation. The overall isothermal crystallization rate of neat PBA and its nanocomposite increases with increasing crystallization temperature. The addition of f-MWCNTs accelerates the isothermal crystallization of PBA as compared with that of neat PBA at a given crystallization temperature, indicative of the nucleating agent effect of f-MWCNTs; however, the crystallization mechanism does not change. The crystal structure of PBA remains unchanged in the PBA/f-MWCNTs nanocomposite despite the presence of f-MWCNTs.     

Studies on the crystallization process of BEA/MOR co-crystalline zeolite

BEA/MOR co-crystalline zeolite was synthesized using tetraethylammonium-fluorides as composite templates. The crystallization process of BEA/MOR co-crystalline zeolite was systematically investigated based on XRD, ICP, SEM, TGA, and nitrogen adsorption characterizations. Through the XRD patterns of the samples with different crystallization times, the BEA and MOR phases did not appear simultaneously in the crystallization process. The BEA phase was the favored product at the beginning of crystallization, whereafter the MOR phase emerged, and the BEA/MOR co-crystalline zeolite was gradually formed. The morphology of obtained particles changed a little during the crystallization process, but the granularity distribution range broadened. Asymmetry of BEA/MOR co-crystalline zeolite particles led to uneven distribution of the mesopores. It is showed that the pore size distribution of the samples with more than 90-h crystallization period exhibited bimodal mesopores distribution, and the pore sizes of the extra mesopores were 4.9 and 5.6 nm, respectively. Based on these results, the crystallization mechanism of BEA/MOR co-crystalline zeolite in tetraethylammonium-fluoride binary templates was roughly proposed.     

The kinetics of isothermal cold crystallization and tensile properties of poly(ethylene terephthalate)

The exothermic peak that is frequently observed during the heating scan of a differential scanning calorimetry (DSC) experiment of poly(ethylene terephthalate) (PET) is due to a cold crystallization process, originating from the rearrangement of amorphous regions into a crystalline phase. In this work the isothermal cold crystallization kinetics of PET was investigated by using DSC, X-ray diffraction and tensile experiments. The isothermal crystallization rate was determined as a function of temperature, and the Avrami analysis was conducted. The results showed that at low temperatures the cold crystallization is a two-regime process, whereas at high temperatures just one stage is observed. The rate constant for isothermal crystallization K increased and the half time of crystallization (t_½) decreased with increasing crystallization temperature. The Avrami exponent n was close to 2, and this corresponds to a disc-like morphology formed by heterogeneous nucleation. Cold crystallization increased the crystallinity and therefore the tensile properties of the samples were enhanced.     

聚乙二醇改性PET／PBT共混体系研究

本文以廉价易得的聚乙二醇(PEG)作结晶促进剂,利用WAXD、DSC研究了PET/PBT共混体系的结晶行为,并以共混体系结晶熔融峰面积计算PET和PBT各自的结晶度。结果发现,加入PEG可以使共混体系冷结晶峰温明显下降,PEG用量越大,冷结晶峰温越低,结晶速度加快;随着PEG分子量增大,当小于2000或等于2000时,冷结晶峰温随之降低,但当分子量≥6000时,冷结晶峰温随之略有升高;加入PEG,对共混体系中PET和PBT各自结晶的作用不同,二者的结晶度随PEG分子量或用量变化不同。     

半结晶性塑料充填数值模拟及温度场分布

从结晶动力学和结晶热力学角度出发,对塑料材料在注塑充填过程中的非等温结晶进行分析,把半结晶性材料在型腔内流动时剪切诱导的结晶对温度场的影响归结到平衡熔融温度的升高上,从而建立从微观到宏观的分析过程.将微观结晶动力学方程与宏观能量方程进行联立,对半结晶性塑料流动过程进行模拟,得到充填结束时的相对结晶度分布,分析其结果表明,把结晶效应考虑到整个充填过程能够得到更准确的温度场计算结果.     

Non-isothermal Crystallization Kinetics of Polyamide 6/Diamine-modified MWNTs Nanocomposite

The non-isothermal crystallization kinetics of polyamide 6/diamine-modified multi-walled carbon nanotube (PA6/D-MWNT) nanocomposite was investigated by differential scanning calorimetry (DSC). The modified Avrami equation, the Ozawa equation and the combined Avrami/Ozawa equation were employed to analyze the non-isothermal crystallization data. The crystallization activation energies were also evaluated by the Kissinger method. It was found that the combined Avrami/Ozawa equation could successfully describe the non-isothermal crystallization process. The results showed that D-MWNTs not only acted as effective heterogeneous nucleating agents for PA6 and noticeably increased the crystallization temperature of PA6, but also influenced the mechanism of nucleation and crystal growth of PA6 and then reduced the overall crystallization rate of the neat PA6 matrix. The crystallization activation energy for the nanocomposite sample was greater than that of the neat PA6, which indicated that the addition of D-MWNTs hindered the mobility of PA6 chain segments.