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－     

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。     

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℃     

Fe73.5Cu1Mo3Si13.5B9微晶软磁合金的结构及其对磁性的影响

对Ｆｅ７３．５Ｃｕ１Ｍｏ３Ｓｉ１３．５Ｂ９微晶软磁合金的结构及其对合金磁性的影响了研究，结果表明，在最佳磁性能下，晶相点阵常数ａ＝０．２８４３ｎｍ，相当于Ｆｅ（Ｓｉ）固溶体中含Ｓｉ％（ｍｏｌ／ｍｏｌ）：１８－２０，体积百分数Ｖ＝７４．８％，晶粒尺寸Ｄ＝１４．６ｎｍ；残余非晶层厚度δ＝１．２３ｎｍ；当Ｔ退火≥５６０℃时明显有Ｆｅ－Ｂ化合物析出。Ｆｅ７３．５Ｃｕ１Ｍｏ３Ｓｉ１３．５Ｂ９合金的磁性不仅与     

快凝钛合金中硅化物的析出及长大规律

研究了热处理对Ｔｉ－５Ａｌ－０．３Ｓｉ和Ｔｉ－５ＡＩ－２Ｚｒ－０．３Ｓｉ（质量分数，ｍｇ／ｇ）析出相长大规律的影响结果表明，含硅的钛合金的快凝态和在６００℃短期（１ｈ）处理后的基体中无析出相＞６５０℃时，近球状的相大量析出热处理后析出相聚集长大速度很快．Ｔｉ－５Ａｌ－０．３Ｓｉ的析出相为四方的Ｔｉ３Ｓｉ，其长大激活能为２１９ｋＪ·ｍｏｌ－１．加入Ｚｒ后，分布更加弥散且长大速度更快的（Ｔｉ，Ｚｒ）６Ｓｉ３的长大激活能为１０５ｋＪ．ｍｏｌ－１     

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．     

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。     

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（ＤＳＣ）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Ｆｅ（７６．５）Ｓｉ（１３．５）Ｂ９Ｃｕ１和Ｆｅ（７３．５）Ｓｉ（１３．５）Ｂ９Ｃ１Ｎｂ３等温晶化的α─Ｆｅ（Ｓｉ）放热峰呈明显的非对称形状     

Zr65Al7.5Ni10Cu15Co2.5合金的玻璃转变温度

根据Ｚｒ６５Ａｌ７。５Ｎｉ１０Ｃｕ１５Ｃｏ２。５合金的纳米晶，晶体，液体和玻璃比热的测量结果，研究了合金的玻璃转变温度与全金的热力学函数，动力学参数以及加热速度的关系。结果表明，非晶态合金玻璃转变所需转变激活能很小，玻璃转变温度实际上是由于加热速度引起的不同状态的玻璃与液体的热力学平衡温度。     

Dielectric properties of K2Zn2(SO4)3 and (NH4)2 Mg2(SO4)3

Dielectric constant (ɛ), dielectric loss (tan δ) and conductivity (σ) for K₂Zn₂(SO₄)₃ and (NH₄)₂ Mg₂(SO₄)₃ have been measured over the frequency range 100 Hz — 100 kHz and in temperature range 30°C — 400°C. The values of static dielectric constant at room temperature are 7.67 and 4.80 for K₂Zn₂(SO₄)₃ and (NH₄)₂ Mg₂(SO₄)₃ respectively. The plots of log σ against reciprocal temperature at different frequencies of these samples merge into a straight line beyond 250°C and the activation energies calculated in this region are found to be 0.67 eV and 1.98 eV for K₂Zn₂(SO₄)₃ and (NH₄)₂ Mg₂(SO₄)₃ respectively.     

Fe_(63)Ni_1Al_5Ga_2P_(9.65)B_(4.6)Si_3C_(6.75)Co_5非晶合金的晶化行为研究

采用XRD、DSC检测技术,采用连续升温晶化和等温退火晶化方法,研究分析了Fe63Ni1Al5-Ga2P9.65B4.6Si3C6.75Co5非晶薄带的晶化动力学行为和晶化过程中晶化相的析出过程。结果表明,该非晶合金的玻璃转变和晶化行为均具有显著的动力学特征。Kissinger法计算得到的Eg、Ex、Ep1、Ep2分别为750、340、432、689kJ/mol,Eg Ex,表明合金具有较好的热稳定性。合金晶化过程为:非晶→非晶+α-Fe→非晶+α-Fe+Fe2P+Fe3P→α-Fe+Fe2P+Fe3P+Fe3C(Al,Si)+Fe5PB2+SiC。合金的晶化类型为初晶型和随后的共晶型反应。     

Dielectric properties of Bi4(GeO4)3 and Bi4(SiO4)3

Dielectric constant, dielectric loss and conductivity of Bi₄(GeO₄)₃ and Bi₄(SiO₄)₃ single crystals have been measured as a function of frequency and in the temperature range from liquid nitrogen temperature to 400° C. The values of the static dielectric constant at room temperature are 16·4 and 13·7 for Bi₄(GeO₄)₃ and Bi₄(SiO₄)₃ respectively. The plots of log (σ) against reciprocal temperature at different frequencies of these crystals merge into a straight line beyond 250°C and the activation energies calculated in this region are found to be 0·95 eV and 1·2 eV for Bi₄(GeO₄)₃ and Bi₄(SiO₄)₃ respectively.     

刚性聚芳醚腈热分解动力学研究

利用ＴＧ,ＤＴＧ方法研究了聚芳醚腈在Ｎ２氢气保不同升温速率β时的热降解过程和动力学。实从难从严当现,随着β的增大,其降解温度呈线性升高, 在空气中的热降解比较,降解率和降解温度的提高。同时,我们利用Ｆｒｅｅｍａｎｃａｒｒｏｌｌ法进行了动力学处理,确定聚芳醚腈在Ｎ２气氛中的热分解为进一步发应,是一级反应,反应活化能为２１０．８ｋＪ／ｍｏｌ。     

Diffusion processes inβ-Zr(Al) phase: a thermodynamic approach

The diffusion behaviour in theβ -Zr(Al) solid solution phase was investigated in the temperature range 1203-1323 K using a thermodynamic approach. The Boltzmann-Matano relation used for determining interdiffusion coefficients and the Darken’s equations used for evaluating the intrinsic diffusion coefficients from velocity of movement of markers in diffusion couples were modified suitably. The composition dependent thermodynamic interdiffusion coefficients were evaluated using chemical potential gradient. Composition and temperature dependence of the thermodynamic interdiffusion coefficients were also established. The thermodynamic intrinsic diffusion coefficients of Al and Zr and their temperature dependence were determined using the modified Darken’s equations.     

Evaluation of the ethylene permeability of polyvinyl chloride (PVC)

The aim of this study was to evaluate ethylene permeation through a food packaging-grade polyvinyl chloride at 3,10,17 and 25°C. The transmission rates were calculated to estimate the permeability (P) at these temperatures. This permeability is influenced by the temperature, giving values from 120 000cm³ μm/m². d atm at 3°C to 367000cm³ μm/m². d atm at 25°C. Other parameters, such as the selectivity factor (p), the temperature coefficient (Q₁₀) and the activation energy (E_a). were compared to values obtained for other gases (O₂ and CO₂) using the same film and supplier.     

Study of non-isothermal kinetics, electrical and optical properties of (GaSeTe) films

Ternary Ga_xSe_86−xTe₁₄ amorphous films (x=15 and 36) were prepared by thermal evaporation. The results of differential scanning calorimetry (DSC) at different heating rates are reported and discussed. The glass transition activation energy, E_t, and the crystallization activation energy, E_c, were evaluated by measuring the heating rate dependence of the glass transition, crystallization onset and peak crystallization temperatures. The average calculated values of E_t and E_c are 140.29 and 97.89 kJ/mol, respectively. The electrical conductivity of amorphous Ga_xSe_86−xTe₁₄ thin films with different thickness has been measured in the temperature range (263.2-333.3 K) and this allows the effect of introducing a metallic impurity to be observed. It was observed that conductivity increases with increasing activation energy and with a lowering of the pre-exponential factor, which suggests the results can be explained in terms of hopping conduction. The optical constants of these films were determined by transmission and reflection measurements at normal incidence in the spectral range of 500-800 nm. The refractive index has anomalous behavior in the spectral range 400-500 nm. The refractive index dispersion can be fitted to a single oscillator model.     

Cd_(1-x)Zn_xS(x=0.88)多晶薄膜的制备及性能研究

采用真空共蒸发法制备了Cd1-xZnxS多晶薄膜,研究了Cd1-xZnxS(x=0.88)多晶薄膜的结构与光电特性。XRD的结果表明,0x≤0.9,Cd1-xZnxS薄膜为六方结构,高度择优取向;荧光光谱分析与Ve-gard定理的结果以及石英振荡法监测的Cd1-xZnxS多晶薄膜的组分吻合;制备的Cd1-xZnxS多晶薄膜的光学透射谱的吸收边随Zn含量的增加发生蓝移,其光学能隙调制在CdS与ZnS能隙之间;最后测量了Cd1-xZnxS薄膜室温电阻率及暗电导率随温度的变化情况,计算了Cd1-xZnxS薄膜的电导激活能。