在Fe-Zn-Mg-Cr尖晶石结构催化剂上丁烯-2氧化动力学

用玻璃外循环无梯度反应器研究了在Fe-Zn-Mg-Cr尖晶石结构催化剂上丁烯-2氧化脱氢动力学。丁烯-2氧化脱氢动力学服从三步骤Redox机理。用脉冲法研究了催化剂用丁烯-2还原及还原催化剂用氧再氧化步骤。用脉冲法测定了丁烯-2吸附热。丁烯-2及丁二烯深度氧化动力学服从经验速度方程。用正交设计法估计了动力学方程的参数。丁烯-2氧化脱氢速度比丁烯-1要快。     

扩展示踪动力学方法的应用：Bi-Mo和铁系尖晶石催化剂上丁烯异构化和氧化脱氢反应动力学性能的比较

以~(14)C标记正丁烯为示踪化合物,用扩展示踪动力学方法解析了在Bi-Mo和铁系尖晶石催化剂上丁烯氧化脱氢全图谱的动力学和反应机理,结果表明,在Bi-Mo催化剂上选择氧化反应速度的顺序为丁烯-1大于丁烯-2,异构化的速度小于选择氧化反应的速度,燃烧反应的速度的顺序也是丁烯-1大于丁烯-2。在铁系尖晶石催化剂上,三种丁烯异构体的选择氧化的速度常数极相近,但顺丁烯略快;它们的异构化速度都明显较小,其中几何异构化的速度大于双键异构化的速度;其燃烧反应速度的次序为丁烯-2>丁二烯>丁烯-1。讨论了工业丁烯氧化脱氢装置中丁烯原料组成的影响,异构化的机理和氧化反应的可能速度控制步骤。     

丁烯氧化脱氢制丁二烯反应中丁烯转化的动力学初步考察

在10毫升催化床的小型装置上进行了丁烯转化动力学的初步考察,以期求出丁烯在L-2605型催化剂上氧化脱氢总包反应的似活化能与反应速度方程. 在排除线速度干扰的情况下,考察了催化剂粒度(粒度平均半径为0.025—0.16厘米)对丁烯氧化盼氢反应中丁烯转化速度的影响.在排除外扩散与内扩散干扰的条件下,进行了反应温度(350—530℃)及各反应物分压(丁烯、丁二烯、氧及水蒸气)对丁烯转化速度的影响的考察.求得丁烯在L-2605型催化剂上氧化脱氢的总包反应似活化能为20.7千卡/克分子.在试验的反应温度范围内,丁烯氧化脱氢中丁烯转化速度方程可表示如r=kp_u,式中r为丁烯转化速度,克分子/小时·克催化剂;k为速度常数,克分子/小时·克催化剂·大气压;p_u为丁烯分压,大气压.     

在 La-Cr-Fe 钙钛矿型催化剂上丁烷、反-2-丁烯及顺-2-丁烯深度氧化动力学

在La-Cr-Fe 钙钛矿型催化剂上用玻璃外循环无梯度反应器研究了丁烷、反-2-丁烯及顺-2-丁烯深度氧化动力学。丁烷、反-2-丁烯及顺-2-丁烯深度氧化动力学服从L-H机理模型。用正交设计法估计了动力学方程中的参数值。丁烷、反-2-丁烯及顺-2-丁烯深度氧化的L-H 机理模型为脉冲实验鉴别。用脉冲色谱法测定了“2-丁烯”及O_2的吸附热。丁烷、反-2-丁烯及顺-2-丁烯深度氧化的CO_2生成速度用(7)式描述。     

钒-铝催化丁二烯、丙烯交替共聚合的动力学研究(Ⅰ)——交替共聚合速度方程

本文研究了VO[OCH₂C(CH₃)₃]₂Cl-Ali-Bu₃催化丁二烯、丙烯交替共聚合的动力学特征,测定了单体和催化剂的反应级数,建立了聚合速度方程,并求得了-80℃-20℃温度范围内的一级速率常数K和总活化能E_T.     

丁烯氧化脱氢催化剂的动力学表征—动力学数据的积分处理方式

本文根据催化剂还原-再氧化机理,推导出丁烯氧化脱氢制丁二烯反应中丁烯总转化的微分和积分动力学方程。用非线性回归法分别关联在锡-磷-锂、钼系七组分及六组分催化剂上的动力学试验数据。估算出相应的动力学参数。此外,还推导出幂式动力学方程的积分表达式,通过数值积分求出原微分方程与试验值的偏差。     

1, 3-丁二烯热裂解的动力学计算与模型研究

1, 3-丁二烯是碳氢燃料燃烧和裂解过程中生成的一种重要产物,也是形成多环芳烃(PAHs)的一种重要前驱体。目前,关于1, 3-丁二烯燃烧实验以及机理的研究较多,但是其热裂解机理的研究较少。本文在B3LYP/CBSB7水平下对1, 3-丁二烯裂解过程中相关反应的反应物、产物以及过渡态进行了几何结构优化和频率计算,并通过组合方法CBS-QB3计算得到了单点能和热力学参数。对于紧致过渡态的反应和无能垒反应,分别采用过渡态理论(TST)和可变反应坐标过渡态理论(VRC-TST)计算其高压极限条件下的反应速率常数。计算得到的反应速率常数与已有文献报导的结果吻合较好。通过量子化学计算,对Hidaka等人提出1, 3-丁二烯的热裂解机理模型进行了更新和改进:更新后的机理模型包含45个物种和224步反应,并对更新后的机理模型进行了模拟验证。结果表明,更新的机理模型能更好地预测1, 3-丁二烯激波管裂解实验过程中C₂H₂、1-丁烯-3-炔(C₄H₄)以及苯(C₆H₆)主要产物的浓度分布,为进一步完善核心机理(C₀-C₄)模型提供了可靠的热、动力学参数。     

扩展示踪动力学方法的应用：用14C标记丁烯-1研究Sn-P-Li催化剂上丁烯氧化脱氢反应中异构化和氧化反应动力学和机理

本文以(14)~C标记丁烯-1在Sn-P-Li催化剂上的异构化和氧化脱氢的机理及动力学为例,详细地介绍了扩展示踪动力学方法。 在Sn-P-Li催化剂上丁烯-1的选择氧化速度明显大于丁烯-2,而燃烧反应的速度却远小于丁烯-2。选择氧化反应对丁烯为0.8级,对氧为0.2级。动力学结果还表明在Sn-P-Li催化剂上丁烯异构化反应主要通过烯丙基脱附进行的。若选择氧化反应是通过烯丙基进行的,则第一个氢原子的裂离可能是速度控制步骤。     

正丁烷在VMgO和Ni-VMgO催化剂上氧化脱氢

 采用4种方法制备了VMgO催化剂样品(w(V2O5)=30%,w(MgO)=70%),并将其用于正丁烷氧化脱氢气固相反应. 结果表明,MgO经蒸馏水回流和焙烧处理后再用NH4VO3溶液浸渍所制得的VMgO,对正丁烷氧化脱氢生成丁烯和丁二烯反应具有更好的催化性能. 这是由于用该法制备的VMgO催化剂中存在较多的Mg3V2O8物种. 通过添加Ni对VMgO催化剂进行了改性. 结果表明,适量添加Ni(n(Ni)/n(V)=0.3)有利于催化剂中Mg3V2O8的生成,而Ni以Ni3V2O8的形态存在. 由此明显改善了VMgO催化剂对正丁烷氧化脱氢生成丁烯和丁二烯反应的催化性能.     

Redox机理动力学内扩散影响的特征

在Pb_0.88Bi_0.06La_0.02Mo/SiO₂催化剂上,反应在动力学区域进行时,甲醇氧化制甲醛服从Redox机理动力学方程:r=(k₁k₂P甲醇Po₂)/(0.5k₁P甲醇+k₂Po₂)当催化剂颗粒增大至3mm时,内扩散影响严重,催化剂有效因子在0.38-0.73之间,其内扩散区域的速度方程为r内=(Do₂/RTKL)2φ_M[K(Po₂-Po_2.o)-ln(1+Kpo₂/1+Kpo_2.o)]^1/2测定了反应受O₂内扩散控制时的反应活化能E内为74.5kJ/mol。     

Effect of ultraviolet irradiation on terpolymerization of sulfur dioxide with two unsaturated compounds

The terpolymerization of sulfur dioxide, butene-1 and acrylonitrile affords terpolymers containing equimolar amounts of sulfur dioxide and butene-1 with various acrylonitrile contents. Ultraviolet irradiation was found to accelerate the polymerization and decrease the acrylonitrile content in the polymer. This fact is interpreted by a mechanism through a copolymerization of sulfur dioxide–butene-1 complex and acrylonitrile, whereby the polymerizability of sulfur dioxide–butene-1 complexed monomer may be accelerated by ultraviolet light. In fact, a binary system of sulfur dioxide and butene-1 was found to be accelerated by ultraviolet irradiation, and it affords a maximum rate at a 1:1 composition of feed monomer. Ultraviolet light of 250–300 mμ wavelength is effective for the initiation and the propagation. This may be ascribed to the ultraviolet absorption of the sulfur dioxide–butene-1 complex. The temperature coefficient was measured in both dark and ultraviolet irradiation reactions. The ultraviolet irradiation enhances the reactivity of sulfur dioxide–butene-1 complexed monomer at low temperature. In the terpolymerization with sulfur dioxide, isoprene, and butadiene, the ratio of isoprene and butadiene in the terpolymer was not altered by ultraviolet irradiation because both monomers from complexes with sulfur dioxide, perhaps having the same temperature coefficient for the polymerization.     

Alternating copolymer of butadiene and propylene. III

Alternating copolymerizations of butadiene with propylene and other olefins were investigated by using VO(acac)₂–Et₃Al–Et₂AlCl system as catalyst. Butadiene–propylene copolymer with high degree of alternation was prepared with a monomer feed ratio (propylene/butadiene) of 4. Alternating copolymers of butadiene and other terminal olefins such as butene-1, pentene-1, dodecene-1, and octadiene-1,7 were also obtained. However, the butadiene–butene-2 copolymerization did not yield an alternating copolymer but a trans-1,4-polybutadiene.     

稀土掺杂对氯化氢氧化制氯气CuO-CeO2-SiO2催化剂结构和性能的影响

采用模板法制备了CuO-CeO₂-SiO₂和稀土掺杂的CuO-Ce_0.9M_0.1O₂-SiO₂ (M=La, Pr, Nd)催化剂. 运用X射线衍射(XRD), N₂吸附-脱附, 透射电镜(TEM), 拉曼(Raman)光谱, X射线光电子能谱(XPS)和氢气-程序升温还原(H₂-TPR)等手段对催化剂的结构进行表征, 并考察稀土掺杂对氯化氢催化氧化制氯气性能的影响. 结果表明, 稀土掺杂进入CeO₂晶格中形成良好的固溶体结构, 获得更小的晶粒尺寸和更高的比表面积, 并且显著提高了固溶体的表面氧空位浓度. 稀土掺杂显著影响了催化剂的氯化氢催化氧化活性, 活性顺序为: CuOCe_0.9La_0.1O₂-SiO₂>CuO-Ce_0.9Nd_0.1O₂-SiO₂>CuO-Ce_0.9Pr_0.1O₂-SiO₂>CuO-CeO₂-SiO₂, 固溶体氧空位浓度的高低与氯化氢氧化活性直接相关. 通过与Ce_0.9M_0.1O₂-SiO₂催化剂的结构和性能的对比, 发现氧空位浓度的提高并不能增强在固溶体表面发生的氯化氢氧化反应. 动力学测试显示, 稀土掺杂后, 氧分子的吸附成为反应过程的决速步骤. 但在V(O₂):V(HCl)=1 条件下, 更高的氧空位浓度导致了固溶体更低的氯化氢氧化反应速率. 结合机理分析认为, CuO-Ce_0.9M_0.1O₂-SiO₂催化剂更高的氧空位浓度增强了固溶体表面的“氧溢流”, 加快了氯化氢氧化的整体反应速率, 这是CuO-Ce_0.9M_0.1O₂-SiO₂具备高活性的关键.     

Anionic Graft Copolymers. III. Hydrogenation of Polydienes Grafted with Vinylaromatics

A new method is described to prepare graft copolymers of polystyrene and polyvinylcyclohexane on polyethylene and poly (ethylene, butene-1). Hydrogenation of the butadiene moieties of graft copolymers of polystyrene on poly-1, 4-butadiene and high vinyl polybutadiene forms graft copolymers of polystyrene on polyethylene and on poly (ethylene, butene-1). Graft copolymers of polyvinylcyclohexane on polyethylene and on poly (ethylene, butene-1) are prepared by completely hydrogenating graft copolymers of polystyrene on poly-1, 4-butadiene and on high vinyl polybutadiene. The physical properties of these polymer systems depend on composition and graft level, resulting in either tough polymers or elastomers.     

An investigation of the structure of butadiene by high resolution infra-red and raman spectroscopy

The rotational Raman spectra of butadiene and butadiene-d₆ are found to consist of discrete lines having small ≈0·4 cm⁻¹) yet almost constant spacings, as would be expected for symmetric or nearly symmetric top molecules. An infra-red absorption band (Type C) of butadiene at 908 cm⁻¹ is observed to have a spacing of about 2·5 cm⁻¹. Both the Raman and infra-red spectra provide evidence for the trans structure of the butadiene molecule. From the rotational constants A″ and ″ the following structural parameters were obtained: C=C---C) = 122·9 ± 0·5° rC---C) = 1·47₆ ± 0·010 Å dy]somewhat shorter than recently determined from electron-diffraction experiments).     

Lifetime and quenching rate constants for a flourescent excited state of tetramethylethylene (2,3-dimethyl-2-butene)

The collisionless lifetime of a flourescent excited state of tetramethylethylene (TME) vapor when excited at 235 nm is 20.8±0.9 ns and the self-quenching rate constant is (2.97±0.01) × 10⁻¹⁰ cm³ molecule⁻¹ s⁻¹. The rate constants for quenching of TME vapor by O₂, benzene. CCl₄, Xe, N₂ and CH₄ are also repeated. In the vapor phase, the lifetime strongly depends on the excitation energy. The lifetime of liquid TME is 10±2 ns at 25±2°C.     

M/(MgO)y(CeO2)1－y(M=Ni、Co、Cu)催化剂的催化甲烷燃烧性能

采用溶胶凝胶法制备了M/(MgO)_y(CeO2)_1－y(M=Ni、Co、Cu)催化剂. 研究了催化剂Ni/(MgO)y(CeO₂)_1－y催化活性与Ce含量的关系, 当y＝0.9时, 催化剂的活性和稳定性最好. 对比研究了(MgO)_0.9(CeO2)_0.1为载体, 负载Ni、Co、Cu活性组分的催化剂催化甲烷燃烧性能. 结果表明, 负载Cu的催化剂活性最好, 但二次评价后催化剂已烧结；负载Ni的催化剂活性与负载Cu的催化剂相差不大, 且稳定性最好, 经1000 ℃焙烧的Ni/(MgO)_0.9(CeO2)_0.1催化剂比表面仍有14.32 m₂•g^－1, 具有较高的催化活性和很好的热稳定性；负载Co的催化剂活性不如前两者, 稳定性居中, 但比表面降低得最少, 抗烧结能力强.     

Effect of the encapsulating material on the peak3/peak5 response ratio of TLD-300 irradiated with neutrons of various energy

The analysis of experimental data available in the literature shows that the neutron sensitivity ratio m=k₃/k₅ for the two main glow peaks P₃ and P₅ of TLD-300 (for ribbons of 3.2×3.2×0.9 mm³) is dependent upon the response ratio R₃/R₅ of these two peaks. This finding is in agreement with predictions from an equation derived from the two-peak method equations. The result implies that the peak response ratio R₃/R₅ for TLD-300 surrounded by Tissue Equivalent material is independent of the encapsulating material. This is also demonstrated experimentally.