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1.
研究了液相沉淀包覆工艺终点pH值对SAPO-34/CZA复合催化剂物化性质和CO2氢还原制低碳烯烃催化性能的影响.借助XRD、SEM、BET、NH3-TPD和CO2-TPD等手段对不同复合催化剂的晶相组成、微观形貌、孔结构及表面酸碱性质进行了分析表征.研究结果表明,沉淀pH值对SAPO-34/CZA复合催化剂物化性质和CO2加氢制低碳烯烃催化性能影响较大.过高或过低的沉淀pH值制得复合催化剂中SAPO-34分子筛结晶度、微孔比表面积及表面碱量均有所下降,呈现以介孔为主的孔结构特征;而当pH值为7时,制得复合催化剂形成了包覆相结构和微-介复合孔结构(微孔比表面积53.1 m2·g-1,介孔比表面积59.8 m2·g-1,总比表面积为112.9 m2·g-1,总孔容0.4 cm3·g-1,平均孔径14.6 nm);在反应温度325℃,还原温度285℃,反应压力3.0 MPa,体积比H2:CO2=3.0,空速3500 mL·g-1·h-1反应条件下,CO2转化率为64.8;,低碳烯烃选择性为49.8;.与pH=9制得催化剂比较,CO2转化率和低碳烯烃选择性分别提高了26.2;和19.2;.  相似文献   

2.
采用等体积浸渍法改性制备了K2 WO4/Al2 O3催化剂,研究了载体Al2 O3晶型对K2 WO4/Al2 O3催化剂物化性质及催化合成甲硫醇的影响.借助XRD、SEM、EDS、BET及NH3/CO2-TPD等手段对不同催化剂的晶相组成、微观形貌、孔结构及表面酸碱性质进行了表征分析.结果表明,Al2 O3晶型对K2 WO4/Al2 O3催化剂晶相组成及微观形貌影响较小,但对孔结构及表面酸碱性质影响较大.与K2 WO4/η-Al2 O3和K2 WO4/θ-Al2 O3催化剂相比,K2 WO4/γ-Al2 O3催化剂具有更大比表面积及孔容(介孔比表面积为226.75 m2·g-1,总孔容为0.557 cm3·g-1),且表面仅有弱酸和弱碱中心(弱酸浓度为0.42521 mmol·g-1,弱碱浓度为0.44184 mmol·g-1).在反应温度370℃,反应压力1.0 MPa,H2 S流速4.9 mL·min-1,CH3 OH流速0.03 mL·min-1反应条件下,K2 WO4/γ-Al2 O3催化剂表现出优良催化性能,甲醇转化率和甲硫醇选择性分别达81.58;和87.05;,与K2 WO4/η-Al2 O3和K2 WO4/θ-Al2 O3催化剂相比,甲醇转化率分别提高了4.23;和19.42;,甲硫醇选择性分别提高了14.68;和7.85;.  相似文献   

3.
采用液相法,以Mg(NO3)2·6H2O为镁源,NH3·H2O为沉淀剂,研究了不同表面活性剂对介孔MgO晶体性质的影响.采用XRD、FT-IR、SEM、BET和CO2-TPD等手段对介孔MgO晶相组成、骨架结构、微观形貌、孔结构及表面化学性质进行了分析表征.研究结果表明,不同表面活性剂对介孔MgO晶体物化性质影响较大.以非离子型PEG-2000为表面活性剂制得产品表面碱强度和碱总量均大于以阴离子型SDS、阳离子型CTAB制得的产品.以非离子型PEG-2000为表面活性剂制备得到的介孔MgO同时具有弱碱、中强碱特征,碱总量为0.192 mmol·g-1,比表面积、孔容和平均孔径分别为145.42 m2·g-1、0.67 cm3·g-1和18.56 nm.  相似文献   

4.
以正硅酸乙酯为硅源,乙醇为溶剂,在溶胶-凝胶法和CO2超临界干燥的基础上,采用分别加入聚乙二醇(400)、六次甲基四胺和尿素作为扩孔剂的方法制备低密度SiO2气凝胶.利用扫描电镜(SEM)、傅里叶变换红外光谱仪(FT-IR)、孔径分布及比表面积测试仪(BET)、纳米压痕仪对未加扩孔剂和加入不同扩孔剂所制备的SiO2气凝胶的表面形貌、结构、比表面积、孔径分布、力学性能以及密度进行研究.结果发现:随着增加扩孔剂的加入量, SiO2气凝胶的密度明显降低;与未加扩孔剂的样品相比,加入扩孔剂所制备的SiO2气凝胶的比表面积和孔径增大;其中,六次甲基四胺具有较佳的扩孔效果,制备得到的SiO2气凝胶的性能较佳,孔径分布主要集中在15~55 nm,平均孔径为35.4 nm,比表面积高达1006 m2· g-1,孔体积为5.3 cm3· g-1,孔隙率高达96.2;.  相似文献   

5.
采用水热包覆法制备了 γ-Al2O3/SAPO-34复合催化剂,考察了γ-Al2O3预处理方式对复合催化剂物化性质和MTO反应催化性能的影响.采用X射线衍射(XRD)、傅里叶红外(FT-IR)、扫描电子显微镜(SEM)、NH3程序升温脱附(NH3-TPD)、N2吸附脱附(BET)等手段对几种复合催化剂进行了分析表征.结果表明,γ-Al2O3预处理方式对复合催化剂物化性质和MTO催化性能影响较大.添加拟勃姆石和电位改性γ-Al2O3制得复合催化剂未形成包覆复合相结构,比表面积较小,表现出较短催化寿命,仅分别为360 min和450 min;添加γ-Al2O3制得复合催化剂形成了包覆相结构和微-介复合孔结构(微孔比表面积123.49 m2·g-1、介孔比表面积122.68 m2·g-1,总比表面积为246.17 m2·g-1,总孔容0.29 cm3·g-1),总酸量较大(0.30 mmol·g-1);在常压、反应温度380℃、进料空速2 h-1反应条件下,复合催化剂催化性能优越,稳定性良好,具有较长的催化寿命,甲醇转化率为100;,低碳烯烃选择性为88.10;,催化寿命达990 min.  相似文献   

6.
利用微波辅助水热合成法直接制备了纳米HZSM-5晶体.采用XRD、FT-IR、SEM、BET和NH3-TPD等手段对合成样品进行了分析表征,研究了晶化温度和时间对合成产物晶体性质的影响.结果表明,晶化温度和时间对微波辅助水热直接合成产物微观形貌、晶粒尺寸和分散度影响明显.较低的晶化温度和较短的晶化时间均难以形成形貌规则的HZSM-5晶体.随着晶化温度的升高,合成样品逐渐变为球形晶粒、晶粒尺寸逐渐增大、分散度逐渐提高,继续提高晶化温度达180 ℃时,晶粒长大使比表面积稍有降低;随着晶化时间的延长,样品的微孔和介孔增多,比表面积和孔容逐渐增大,继续延长晶化时间,晶体内微孔可能的收缩和晶粒的长大使得样品孔容和比表面积减小.160 ℃和1.5 h条件下制备的HZSM-5分子筛晶体形貌呈球形,晶粒尺寸约为60 nm,分散程度较好;其比表面积、孔容和平均孔径分别为398.45 m2·g-1、0.63 cm3·g-1和6.27 nm;晶体表面具有弱酸特征.  相似文献   

7.
采用水热包覆法制备了ZrO2/SAPO-34复合催化剂,研究了ZrO2预处理方式对复合催化剂物化性质和MTO催化性能的影响.采用XRD、FT-IR、SEM、NH3-TPD和BET等手段对不同复合催化剂的晶相组成、骨架结构、微观形貌、表面酸性质及孔结构进行分析表征.结果表明,ZrO2预处理方式对复合催化剂物化性质和MTO催化性能影响较大.未焙烧和焙烧经聚电解质改性ZrO2制得复合催化剂未形成连续复合相,比表面积小,表现出较短的催化寿命,仅为410 min和530 min;450℃焙烧ZrO2制得复合催化剂形成了均匀连续复合相和层级结构孔特征(微孔比表面积112.91 m2· g-1,介孔比表面积176.02 m2· g-1,总比表面积为288.93 m2· g-1,总孔容0.19 cm3· g-1),总酸量较大(0.344 mmol/g);在常压、反应温度380 ℃、N2流速20 mL· min-1、进料空速2 h-1MTO反应条件下,复合催化剂表现出优越催化性能、稳定性及反应寿命,甲醇转化率和低碳烯烃选择性分别达100;和90.54;,催化寿命达1130 min,与单一SAPO-34分子筛相比,催化寿命延长了768 min.  相似文献   

8.
以间苯二酚-甲醛为碳源前驱体,正硅酸乙酯为硅源前驱体,嵌段聚合物F127(PEO106PPO70PEO106)为模板剂,在酸性条件下采用三组分共组装制备了具有介孔结构的碳硅复合材料.通过NaOH清洗去除硅元素可以得到具有更高面积和孔容的介孔碳.TEM和小角XRD结果表明,添加了正硅酸乙酯后所得介孔材料由有序结构变为无序蠕虫状.介孔碳材料的比表面积由389 m2/g增加到602 m2/g,孔容由0.45 cm3/g增加到0.58 cm3/g.所得介孔材料对溶菌酶的吸附量随着介孔材料比表面积和孔容的增加而增大.纯介孔碳的吸附行为符合Langmuir等温线吸附拟合,高比表面介孔碳的吸附过程符合Freundlich等温线吸附拟合.  相似文献   

9.
采用共沉淀包覆法制备了SAPO-34/CZA双功能复合催化剂,研究了复合相比例对催化剂晶体结构性质和CO2加氢制低碳烯烃催化性能的影响.采用XRD、FT-IR、SEM、BET、NH3-TPD和CO2-TPD等手段对不同催化剂的晶相组成、骨架结构、微观形貌、孔结构及表面酸碱性进行了分析表征.研究结果表明,复合相比例对SAPO-34/CZA双功能复合催化剂的结构性质和催化性能影响较大.质量比为1∶1时,制得复合催化剂具有明显微孔和介孔特征(微孔比表面积53.15 m2·g-1、介孔比表面积59.84 m2·g-1、总比表面积为113.00 m2·g-1、总孔容0.41 cm3·g-1、平均孔径14.57 nm),具有特殊包覆结构及存在复合相界面,构造了特殊反应路径,微介孔层级结构强化耦合反应,表现出较高催化性能.在还原温度285 ℃、反应温度325 ℃、压力3.0 MPa、V(H2)/V(CO2)=3.0、空速(SV)3500 mL·g-1·h-1的条件下,CO2转化率为64.80;,低碳烯烃选择性为49.68;.与物理共混催化剂SAPO-34/CZA-M相比,CO2转化率和低碳烯烃选择性分别提高了31.98;和2.43;.  相似文献   

10.
以高锰酸钾(KMnO4)和聚乙烯吡络烷酮(PVP)为原料,采用氧化还原法制备介孔氧化锰.研究发现,产物的晶型和微观结构受KMnO4溶液浓度的影响.当KMnO4溶液浓度从0.1 mol·L-1增加到0.3 mol·L-1,产物从比表面积13.6 m2·g-1的晶态Mn3O4转变成比表面积约60 m2·g-1的非晶态MnO2.电化学测试表明:非晶MnO2具有最佳电化学性能,在2 mol·L-1 KOH溶液中,1 A·g-1的电流密度下的比电容可达442 F·g-1,5 A·g-1的电流密度下循环1100次后比电容保有率为72.6;.  相似文献   

11.
The evolution of the geometric characteristics introduced by Pauling and their dependence on the specific features of the structure and chemical bonds have been considered. The values of the covalent and van der Waals radii are given as well as their relationships and mutual transitions.  相似文献   

12.
Rakin  V. I. 《Crystallography Reports》2020,65(6):1033-1041
Crystallography Reports - The relationship of morphological spectra (sets of data on the morphological types of real polyhedral crystals and their probabilities under current physicochemical...  相似文献   

13.
SAXS in situ experiments on the evolution of TMOS solutions during hydrolysis and polycondensation lead to power laws with scaling exponents ≈ 2. It is suggested that this could be the result of the polydispersity of the samples and that only an apparent fractal dimension can be obtained in this way. Kinetic studies tend to indicate that agglomeration in the sol is the result of a diffusion-controlled process.  相似文献   

14.
We investigate the possibility of controlling the curvature parameters of parabolic mirrors that are modular elements of two types consisting of a base and thin inserts placed at the opposite side of the work surface. In the first type of modular elements, bending is controlled by the difference in the coefficients of the thermal expansion of the base and inserts. In the second type of elements, the profile is changed by the piezoelectric straining of the inserts under an electric field. A correlation is established between the parameters of modular elements and their surface curvature profile.  相似文献   

15.
A review of measurement of thermophysical properties of silicon melt   总被引:2,自引:0,他引:2  
Measurements of thermophysical properties of Si melt and supplementary study of X-ray scattering/diffraction by the authors' group were reviewed. The values obtained differed variously from those of literature. Density was 2–3% larger, surface tension 20–30% smaller, viscosity up to 40% larger, electrical conductivity 8% smaller, spectral emissivity more or less in good agreement with literature values, and thermal diffusivity a few percent larger. An anomalous density jump was found near the melting point. Surface tension and viscosity also showed anomaly. A strange time-dependent change of density was observed over 3 h after melting. X-ray analyses suggested a slight change in local atom ordering, but showed no sign of cluster formation. An addition of 0.1 at% gallium caused the density jump to disappear, while that of boron caused no change. An EXAFS study of the former melt indicated a strong interaction between Ga and Si atoms as if molecules of GaSi3 existed. The implications of the measured properties are a possibility of soft-turbulence in an Si melt in a relatively large crucible, a more complicated manner of intake of oxygen depleted molten Si from the free surface region to underneath the growing crystal, and a relaxation of the melt after melting arising from trapped gas species.  相似文献   

16.
Within the method of discrete modeling of packings, an algorithm of generation of possible crystal structures of heteromolecular compounds containing two or three molecules in the primitive unit cell, one of which has an arbitrary shape and the other (two others) has a shape close to spherical, is proposed. On the basis of this algorithm, a software package for personal computers is developed. This package has been approved for a number of compounds, investigated previously by X-ray diffraction analysis. The results of generation of structures of five compounds—four organic salts (with one or two spherical anions) and one solvate—are represented.  相似文献   

17.
Crystal chemical characteristics of the α and β modifications of Zn2V2O7 are calculated based on in situ high-temperature X-ray measurements. The expansion of the structure is found to be strongly anisotropic up to the negative volumetric thermal expansion of the α-Zn2V2O7 unit cell in the temperature range of 300–600°С, α V =–17.94 × 10–6 1/K. The transformations of the “hard” and “soft” sublattices with an increase temperature and at the phase transition are considered in detail. It is shown that the negative volumetric thermal expansion of α-Zn2V2O7 is due to the degeneracy of the zigzag-like shape of zinc–oxygen columns at constant distances between their vertices.  相似文献   

18.
Crystallography Reports - Macroscopic jumps of plastic deformation (few percent in amplitude) on creep curves of aluminum–magnesium alloy, caused by a local effect of concentrated solution of...  相似文献   

19.
I. Avramov 《Journal of Non》2011,357(22-23):3841-3846
The temperature dependence of viscosity of silicate melts is discussed in the framework of the Avramov–Milchev (AM) equation. The composition is described by means of two parameters: the molar fraction, x, and the “lubricant fraction”, l. The molar fraction is the sum of the molar parts xi of all oxides dissolved in SiO2, the molar fraction of the latter being 1 ? x. It is shown that, with sufficient precision, two of the parameters of the AM equation can be presented as unique functions of the molar fraction. On the other hand, x is not sufficient to determine properly the reference temperature Tr , at which viscosity is ηr = 1013 [dPa.s]. Therefore, additional parameter, “lubricant fraction” l, is introduced. For each of the components, li is a product of molar part xi and a specific dimensionless coefficient 0  ki  1 accounting for the specific contribution of this component to the increased mobility of the system. It is demonstrated that, for l > 0, the reference temperature is related to the “lubricant fraction” l through the reference temperature Tr,SiO2 of pure SiO2.  相似文献   

20.
Two types of domain-wall equations are analyzed: the equations derived by the Sapriel method and the equations obtained by interface matching of the thermal-expansion tensor. It is shown that, for W-type domain walls, these methods yield the same equations. For W′-type domain walls, the equations obtained by different methods coincide for proper ferroelastics and differ for improper ferroelastics.  相似文献   

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