爆轰裂解法制备纳米石墨粉的吸附性能研究(英文)

在酸含量不同的原材料中,通过爆轰的方法制备纳米石墨粉,并利用BET方程以及BJ H方法对所得纳米石墨粉进行比表面积和孔径分布分析。分析结果表明,所得爆轰产物中有的比表面积大致为天然鳞片石墨的5.3~9.2倍,而且随酸含量的增大逐渐增大,产物的等温线中存在吸附滞后现象。其中,增大的比表面积主要由分布在3 nm至7 nm之间的孔引起的,而且在爆轰后,孔径4 nm左右的孔,其数量达到最大值。通过对纳米石墨粉的研究,分析了酸在爆轰过程中的积极作用,并为纳米石墨粉的进一步应用提供了结构信息。     

炸药爆轰法制备纳米石墨粉及其在高压合成金刚石中的应用

介绍了一种制备纳米石墨粉的新方法——负氧平衡炸药爆轰法. 对合成的黑粉产物进行x射线衍射分析，确认其为石墨结构，平均晶粒度为2.58 nm. 透射电子显微分析的结果表明，炸药爆轰法制备的黑粉为六方结构的纳米石墨粉，颗粒呈球形或椭球形. 用小角x射线散射法测定纳米石墨粉的粒度分布在1—50 nm，有92.6wt%的粉末粒度小于16 nm. 平均粒径为8.9 nm. 纳米石墨粉的比表面积约为500—650 m²/g. 在六面顶压机中用纳米石墨粉在Fe粉触媒的作用下进行金刚石的高压合成实验 关键词： 纳米石墨粉 爆轰 金刚石 合成     

炸药爆轰制备纳米石墨粉储放氢性能实验研究

介绍了一种新的制备纳米石墨粉的方法——炸药爆轰法.通过对爆轰合成的黑色粉末进行x射线衍射分析，确认其为六方结构的纳米石墨，平均晶粒度为1.86—2.61nm.用BET气体吸附仪测试纳米石墨粉的比表面积约为500—650m2/g，由比表面积计算得到的纳米石墨粒度为4.41—6.85nm.在室温（≈290K）和12MPa压力条件下对纳米石墨粉进行储放氢气性能测试，结果表明纳米石墨粉样品的储放氢量为0.33wt%—0.37wt％.在相同实验条件下，纳米石墨粉原始样品的储放氢能力较原始纳米炭纤维（0.15wt%—0.35wt％）和多壁碳纳米管（0.15wt%—0.20wt％）的储放氢能力略强,但低于超级活性炭（0.92wt%—0.98wt％）.纳米碳材料的比表面积在其储放氢实验中起关键作用. 关键词： 爆轰 纳米石墨粉 比表面积 储放氢量     

五羰基铁气相爆轰法合成纳米碳胶囊

采用气相爆轰法,以乙炔气体、氧气和五羰基铁为原料成功地合成了比表面积为253.857m~2/g的胶囊状碳纳米材料。对反应的前置实验九羰基二铁的热分解反应的研究表明,在60～140℃之间,九羰基二铁热分解为五羰基铁和十二羰基三铁。对爆轰产物进行了XRD、TEM和BET物理吸附实验,结果表明:产物XRD图谱石墨峰明显,产物主要为具有石墨化倾向的薄层胶囊状无定形碳结构;实验产物比表面积为253.857m~2/g,孔体积为0.940cm~3/g,平均孔径为2.731nm;吸附-脱附曲线回滞环类型为H3型,孔结构主要为颗粒堆积而形成的狭缝孔;爆轰产物比表面积较大,具有较强的吸附能力。证实了同样采用铁作为触媒,乙炔在不添加惰性气体作为缓冲剂的情况下,由于爆速过高而无法用于合成碳纳米管。     

气相/凝聚炸药爆轰合成的碳包铜纳米颗粒特征

采用凝聚炸药爆轰和气相爆轰分别制备碳包铜纳米颗粒,并利用XRD,Raman和TEM等方法对合成纳米产物进行对比分析。其中凝聚炸药爆轰法以柠檬酸铜干凝胶、油酸和黑索金为原料按照一定比例配成爆炸源,在氮气的保护氛围中引爆；而气相爆轰法以乙酰丙酮铜为原料,分别以H2和O2,H2和空气为爆炸源,在负氧条件下引爆。通过XRD,Raman和TEM分析结果表明,两类爆轰法均可得到分散性良好的碳包覆铜纳米颗粒,碳壳石墨化程度较高。气相爆轰可以合成10 nm以下的纳米晶粒,而凝聚炸药爆轰合成的晶粒尺寸在20~40 nm,且存在较多空壳结构；气相爆轰产物其碳壳尺寸在2~3 nm,凝聚炸药爆轰产物其碳壳尺寸在2~5 nm。     

压汞法分析生物质焦孔隙结构

对于稻壳、树叶、棉花杆、玉米杆四种生物质焦,通过压汞法测量了其在大孔和部分中孔范围内的孔隙结构,发现热解温度、热解保持时间、热解快／慢速都会影响着焦样的比表面积和平均孔径。四种生物质中,树叶焦样的比表面积最大,玉米杆的比表面积最小;稻壳焦样的平均孔径最小,玉米杆的平均孔径最大。不同生物质焦样的孔径分布规律有很大不同。热解温度、热解速度和热解保持时间对孔径分布规律的影响不大,决定孔径分布规律的是生物质本身。在中孔和大孔的范围内,四种生物质焦样的孔径分布曲线都呈现出双峰结构。     

炸药爆轰法制备的纳米石墨粉的拉曼光谱

负氧平衡炸药爆轰法合成的纳米石墨粉,是一种新型的具有良好实用前景的纳米粉体材料。采用负氧平衡炸药梯恩梯(TNT),在分别充有氮气、氩气、二氧化碳等保护性气体、压力为0.25～2 atm的密闭容器内爆轰制备了纳米石墨粉。用激光拉曼光谱对制备的样品进行了测试,结果表明样品为石墨结构。纳米石墨粉的Raman峰与块体石墨相比,其峰位向高波数方向偏移了约5 cm-1。纳米石墨粉Raman峰的半高宽约为22 cm-1,由此可计算出纳米石墨粉的颗粒大小为2.97～3.97 nm。与高纯石墨Raman峰相比,纳米石墨粉的Raman峰由于尺寸效应出现了蓝移现象, 并对此现象进行了讨论。用X射线衍射仪(XRD)和透射电子显微镜(TEM)测定了纳米石墨粉的物相,并对其颗粒粒径进行了估算,其结果为2.58 nm(酸处理前)和1.86 nm(酸处理后),与Raman光谱的结果基本吻合。     

纳米二氧化钛粉体的气相爆轰制备

 介绍了利用氢氧混合气体为原料、以四氯化钛为前驱体、气相爆轰制备纳米二氧化钛粉体的方法。利用XRD衍射结果分析证明，产物为金红石相和锐钛矿相的二氧化钛混晶，其晶粒尺度为纳米量级。通过XRD、SEM、TEM分析可以得出，粒子基本为球形，大部分粒子粒径为10~20 nm，也有少量的100 nm左右的粒子产生。分析后发现，反应发生在爆燃转爆轰的过程中和爆轰管中的湍流现象是导致大粒子产生的主要原因。在对在氢过量和氧过量两种状况下，对爆轰所产生的产物的形貌进行了对比，分析发现两种状况产生纳米二氧化钛粉末粒径分布和形貌并没有太大变化。     

介孔二氧化钛光催化降解乙醛及其影响因素

"应用溶剂蒸发自组装的方法合成了具有蠕虫状孔道的介孔二氧化钛粉末和薄膜．考察了不同焙烧温度对材料介孔结构和光催化性能的影响．乙醛光催化降解实验用来表征不同焙烧温度下介孔材料的光催化性能．结果表明实验中合成的介孔二氧化钛材料的光催化活性明显高于颗粒二氧化钛(Degussa P25)．其中400 oC焙烧的样品具有平均孔径为6.0 nm的窄的孔径分布和117 m2/g的大的比表面积．通过对光催化活性结果的分析,发现介孔二氧化钛的活性主要受其比表面积和结晶性的共同影响．对介孔二氧化钛薄膜材料进行了同样的光催化表     

爆轰合成碳包覆钴、镍磁性纳米颗粒的探索

 介绍了爆轰法合成碳包覆钴、镍纳米磁性颗粒研究的初步结果。以黑索今炸药为主体,加入钴、镍金属硝酸盐与有机碳源材料,在爆炸容器中氮气保护下用导爆管雷管引爆,成功地合成了碳包覆钴、镍纳米磁性颗粒。为了探求爆轰固体产物的形貌特征及性能,分别采用了TEM、XRD、VSM等测试手段对其进行表征。实验结果表明,爆轰产物中主要含有碳包覆纳米钴、纳米镍磁性颗粒,成球体或者椭球体,具有完好的核壳结构形貌。合成的碳包覆钴颗粒分布在30~50 nm之间,碳包覆的镍颗粒分布在25~60 nm之间,外层碳壳层主要由无定形碳和石墨构成。磁性测试表明,所得碳包金属钴、镍颗粒在室温下具有良好的软磁特性。     

Synthesis and characterization of copper oxide (I) nanoparticles produced by pulsed sonoelectrochemistry

Cu(2)O nanopowders have been prepared by ultrasound-assisted electrochemistry with a potentiostatic set-up. Their composition has been determined by X-ray diffraction and energy dispersive X-ray spectroscopy. Transmission electron microscopy and centrifugation analyses indicate that the nanopowders consist of agglomerates of variable nanometric diameter grain. Most of particles have a diameter of 8 nm whatever the electrodeposition potential. The influence of the parameters of electrochemical and ultrasonic pulses on the particle diameter was also studied. The specific surface areas determined by Brunauer-Emmet-Teller (BET) model are very high with a value close to 2000 m(2)g(-1).     

BET surface area of carbonaceous adsorbents—Verification using geometric considerations and GCMC simulations on virtual porous carbon models

The applicability of BET model for calculation of surface area of activated carbons is checked by using molecular simulations. By calculation of geometric surface areas for the simple model carbon slit-like pore with the increasing width, and by comparison of the obtained values with those for the same systems from the VEGA ZZ package (adsorbate-accessible molecular surface), it is shown that the latter methods provide correct values. For the system where a monolayer inside a pore is created the ASA approach (GCMC, Ar, T = 87 K) underestimates the value of surface area for micropores (especially, where only one layer is observed and/or two layers of adsorbed Ar are formed). Therefore, we propose the modification of this method based on searching the relationship between the pore diameter and the number of layers in a pore. Finally BET; original and modified ASA; and A, B and C-point surface areas are calculated for a series of virtual porous carbons using simulated Ar adsorption isotherms (GCMC and T = 87 K). The comparison of results shows that the BET method underestimates and not, as it was usually postulated, overestimates the surface areas of microporous carbons.     

Adsorption of argon and nitrogen in cylindrical pores of MCM-41 materials: application of density functional theory

Adsorption of argon and nitrogen at their respective boiling points in cylindrical pores of MCM-41 type silica-like adsorbents is studied by means of a non-local density functional theory (NLDFT), which is modified to deal with amorphous solids. By matching the theoretical results of the pore filling pressure versus pore diameter against the experimental data, we arrive at a conclusion that the adsorption branch (rather than desorption) corresponds to the true thermodynamic equilibrium. If this is accepted, we derive the optimal values for the solid-fluid molecular parameters for the system amorphous silica-Ar and amorphous silica-N₂, and at the same time we could derive reliably the specific surface area of non-porous and mesoporous silica-like adsorbents, without a recourse to the BET method. This method is then logically extended to describe the local adsorption isotherms of argon and nitrogen in silica-like pores, which are then used as the bases (kernel) to determine the pore size distribution. We test this with a number of adsorption isotherms on the MCM-41 samples, and the results are quite realistic and in excellent agreement with the XRD results, justifying the approach adopted in this paper.     

One-pot sonochemical fabrication of hierarchical hollow CuO submicrospheres

Hierarchical hollow CuO submicrospheres have been fabricated on a large scale by a facile one-pot sonochemical process in the absence of surfactants and additives. The as-prepared products were investigated by XRD, FESEM, EDX, TEM, SAED, HRTEM and BET nitrogen adsorption-desorption isotherms. The results reveal that hollow pumpkin-shaped structures possess a monoclinic phase CuO with the diameters ranging from 400 to 500 nm, and their walls with around 45 nm in thickness are composed of numerous single crystalline CuO nanoribbons with a width of about 8 nm. The BET specific surface area of the as-synthesized CuO hollow structures was measured to be 59.60 m(2)/g, and the single point adsorption total pore volume was measured to be 0.1036 cm(3)/g. A possible growth mechanism for the formation of hierarchical hollow CuO structures was proposed, which is considered to be a sonohydrolysis - oriented aggregation - Ostwald ripening process. The novel hollow CuO spherical structures may utilize applications in biosensors, photonics, electronics, and catalysts.     

MF气凝胶的制备和结构表征

 以三聚氰胺(M)和甲醛(F)为原料，经溶胶-凝胶和超临界干燥工艺制备出密度156.82 mg/cm³的MF气凝胶。通过X射线衍射仪(XRD)、扫描电镜(SEM)、透射电镜(TEM)及比表面测定仪(BET)等测试手段研究了其结构和性能。XRD结果表明MF气凝胶是一种非晶材料；TEM和SEM结果表明MF气凝胶所有孔孔径均在10 nm左右；孔径分布及比表面积测试仪测得该气凝胶具有很高的比表面积（1 015.98 m²/g），孔径大小主要为5~30 nm。所得MF气凝胶是一种具有nm量级3维网络结构的轻质多孔材料，有望在ICF实验靶中得到应用。     

Excess surface work—A modelless way of getting surface energies and specific surface areas directly from sorption isotherms

Sorption isotherms can be easily transformed into excess surface work (ESW) isotherms, computed as the product of the adsorbed amount and the change in chemical potential. Plotted against the amount adsorbed at least one minimum is yield. Thermodynamically ESW is the sum of the surface free energy and the isobaric isothermal work of sorption. Therefore, ESW is not a model, instead it is just another way of presenting an isotherm. From the amount adsorbed in the first minimum one can obtain a specific surface area similar to the BET surface area. The depth of the ESW in the minimum gives a sorption energy, which corresponds approximately to the loss of degrees of freedom of the sorptive. In this contribution the ESW plots of various sorption isotherms on highly ordered alumina with cylindrical pores of 25 nm width and mesoporous SBA 15 will be presented and discussed.     

Template synthesis of nanostructured silica with hollow core and mesoporous shell structures

Silica capsules with hollow macroporous core–mesoporous shell (HCMS) were synthesized through template-assisted replication of submicrometer-size polystyrene spheres as templates. The silica mesoporous shell exhibited highly ordered hexagonal structure as confirmed by X-ray diffraction pattern and TEM image. The pore diameter and BET surface area of this sample were found to be 2.1 nm and 1387 m²/g, respectively.