CN1488462A - A method for tailoring and coating nanoparticle surface physicochemical structure - Google Patents
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Abstract
一种纳米粒子表面物理化学结构裁剪包覆方法。通过对射频等离子体进行调制,控制脉动比、时间、功率等放电条件,进而控制官能团的种类、含量、沉积层厚度、包膜的粗糙度等,可在包覆对象例如TiO2等纳米粒子表面选择性“裁剪”包覆具有特定单体分子官能团的薄膜,并调控包覆层的厚度、表面粗糙度等物理形态,获得具有特定物理、化学结构的包覆膜,改变纳米粒子的表面物理化学结构。与传统的包覆方法比较,本方法具有干态、常温、环境污染小、膜层均匀、厚度可控、包覆层和纳米芯核结合紧密、单体选择范围广等优势。它可通过空间物理位阻与化学相容性,降低纳米粒子的团聚性,以体现小尺寸给纳米粒子带来的特殊效应。也可用于纳米复合颗粒的研制等。A method for tailoring and covering the surface of nanoparticles with physical and chemical structures. By modulating the radio frequency plasma, controlling the pulse ratio, time, power and other discharge conditions, and then controlling the type and content of functional groups, the thickness of the deposited layer, the roughness of the coating, etc., it can be coated on the surface of nanoparticles such as TiO 2 Selectively "cut" the coating film with specific monomer molecular functional groups, and control the physical form such as the thickness and surface roughness of the coating layer, obtain a coating film with a specific physical and chemical structure, and change the surface physical and chemical properties of nanoparticles structure. Compared with the traditional coating method, this method has the advantages of dry state, normal temperature, less environmental pollution, uniform film layer, controllable thickness, tight combination of coating layer and nano core, and wide range of monomer selection. It can reduce the agglomeration of nanoparticles through steric physical hindrance and chemical compatibility, so as to reflect the special effect of small size on nanoparticles. It can also be used in the development of nanocomposite particles, etc.
Description
技术领域technical field
本发明涉及利用等离子体放电方法在纳米粒子表面包覆一层薄膜的方法。具体的是关于一种纳米粒子表面物理化学结构裁剪包覆方法,是在真空等离子体条件下通过对脉动射频等离子体进行放电参数的调制,按照包覆对象的不同,选择性地裁剪设计包覆膜的化学物理结构,从而达到裁剪设计纳米粒子的表面物理化学结构的目的。The invention relates to a method for coating a layer of thin film on the surface of nanoparticles by using plasma discharge method. Specifically, it relates to a method of tailoring and coating the physical and chemical structure of the surface of nanoparticles, which is to modulate the discharge parameters of the pulsating radio frequency plasma under vacuum plasma conditions, and selectively tailor and design the coating according to the different coating objects. The chemical and physical structure of the film, so as to achieve the purpose of tailoring the surface physical and chemical structure of nanoparticles.
背景技术Background technique
目前,各种结构类与功能类纳米粒子材料的研究与应用正引起越来越多的关注。形成纳米复合材料时,只有当其中任一相的尺寸达到100纳米以下或更低时,其小尺寸带来的特异功能性才能体现。但此时,表面原子占总原子数的比例激增,表面能迅速增大,粒子的团聚现象愈加严重,因而要使纳米粒子在基体中达到纳米级的分散很难。At present, the research and application of various structural and functional nanoparticle materials are attracting more and more attention. When forming nanocomposites, only when the size of any one of the phases reaches 100 nanometers or less, the specific functionality brought by its small size can be realized. But at this time, the proportion of surface atoms to the total number of atoms increases sharply, the surface energy increases rapidly, and the agglomeration of particles becomes more serious, so it is difficult to achieve nanoscale dispersion of nanoparticles in the matrix.
由于纳米材料分散性能很大程度上受纳米粒子表面性能影响,因而表面改性是常用的改进纳米粒子分散性的方法之一,对纳米材料体现其特异功能至关重要。各种液态方法,如偶联剂、表面活性剂、有机低聚物等,主要通过改变表面化学结构改善纳米粒子的分散性。但应用中存在使用温度低,包覆过程需要反复进行固液分离操作等不足。气态方法如激光溅射、等离子体包覆等,可以通过简单的一步法进行包覆。等离子体包膜是通过放电裂解各类聚合或非聚合性的单体,气相聚合沉积,通过反应活性种与纳米粒子表面的物理和化学结合,在纳米粒子表面包覆极薄的一层膜。目前国内外正开始这方面的研究,如D Shi等应用射频连续波等离子体聚合方法,在尺寸10nm到150nm的Al2O3和ZnO纳米粒子表面获得极薄的均匀薄膜(D Shi etal.,Appl.Physics Letter,2001,78(9):1243-1245);Dorothee V.Szabo等用微波等离子体在Fe3O4纳米粒子表面包覆聚甲基丙烯酸甲酯(PMMA)薄膜(Dorothee V.Szabo et al.,Advanced Materials,1999,11(15):1313-1316)。上述纳米粒子的等离子体包覆大都使用射频连续波等离子体方法,它对单体原有结构破坏极大,较难保留原有单体含氧、含氮等的官能团,如COOH、OH、NH2等,聚合包覆得到的膜层有很高的交联度,因此渗透性很低,而且不溶不熔,在调控沉积膜化学结构方面灵活性小。最近发展起来的脉动射频等离子体在材料表面改性方面,可通过对射频等离子体进行脉动调制,使放电在“开”与“关”之间间歇进行,“开”时产生自由基,在“关”的间歇,可以进行常规自由基聚合,从而可选择性地“裁剪”保留特定的单体分子官能团。如Licheng M.Han等人将其用于全氟烷基苯在平面玻璃或硅片上的膜沉积,选择性保留单体中耐热苯环和对绝缘性能有贡献的CF官能团,获得低介电常数和高热稳定性的功能膜涂层(Licheng M.Han,et al.,1997,Langmuir,13:5941)。张菁等在乙烯基乙酸脉动射频等离子体聚合的研究中,当脉动比减小时,玻片上聚合膜结构中羧基、羟基的含量呈上升趋势(张菁等,物理学报,2003,52(7):1707-1712)Since the dispersion performance of nanomaterials is largely affected by the surface properties of nanoparticles, surface modification is one of the commonly used methods to improve the dispersion of nanoparticles, which is very important for nanomaterials to exhibit their specific functions. Various liquid methods, such as coupling agents, surfactants, organic oligomers, etc., mainly improve the dispersion of nanoparticles by changing the surface chemical structure. However, in the application, there are disadvantages such as low operating temperature and repeated solid-liquid separation operations during the coating process. Gaseous methods such as laser sputtering, plasma coating, etc., can be coated in a simple one-step process. Plasma coating is to crack various polymeric or non-polymerizable monomers by discharge, and then vapor phase polymerization deposition. Through the physical and chemical combination of reactive species and the surface of nanoparticles, a very thin layer of film is coated on the surface of nanoparticles. At present, research in this area is beginning at home and abroad. For example, D Shi et al. applied radio frequency continuous wave plasma polymerization method to obtain extremely thin uniform films on the surface of Al2O3 and ZnO nanoparticles with a size of 10nm to 150nm (D Shi et al., Appl.Physics Letter, 2001,78 (9): 1243-1245); Dorothee V.Szabo etc. use microwave plasma to coat polymethyl methacrylate (PMMA) film on the surface of Fe 3 O 4 nanoparticles (Dorothee V. Szabo et al., Advanced Materials, 1999, 11(15):1313-1316). The plasma coating of the above-mentioned nanoparticles mostly uses the radio frequency continuous wave plasma method, which greatly damages the original structure of the monomer, and it is difficult to retain the functional groups containing oxygen and nitrogen of the original monomer, such as COOH, OH, NH 2, etc., the film layer obtained by polymer coating has a high degree of crosslinking, so the permeability is very low, and it is insoluble and infusible, and has little flexibility in regulating the chemical structure of the deposited film. The recently developed pulsating radio frequency plasma can be used to modify the surface of materials by pulsating the radio frequency plasma, so that the discharge can be performed intermittently between "on" and "off". In the interval of "off", conventional free radical polymerization can be carried out, so that specific functional groups of monomer molecules can be selectively "tailored". For example, Licheng M.Han et al. used it for the film deposition of perfluoroalkylbenzene on flat glass or silicon wafers, selectively retaining the heat-resistant benzene ring in the monomer and the CF functional group that contributes to the insulation performance, and obtained low dielectric properties. Functional film coatings with electrical constant and high thermal stability (Licheng M. Han, et al., 1997, Langmuir, 13:5941). In the research of pulsating radiofrequency plasma polymerization of vinyl acetic acid by Zhang Jing et al., when the pulsation ratio decreases, the content of carboxyl and hydroxyl groups in the polymeric film structure on the glass slide tends to rise (Zhang Jing et al., Acta Physica Sinica, 2003, 52(7) : 1707-1712)
然而,利用等离子体聚合方法进行纳米粒子包覆还存在着如何对单一粒子而非粒子团聚体进行包覆的难题。由于前述纳米粒子的表面能很高等原因,纳米粒子极易产生团聚,要在单个的纳米粒子而非粒子的团聚体表面进行包覆就显得异常困难。而且在等离子体聚合方法进行纳米粒子包覆时,选择性地“裁剪”保留特定的单体分子官能团,也是有待解决的问题。However, there is still a problem of how to coat single particles instead of particle aggregates in the coating of nanoparticles by plasma polymerization. Due to the high surface energy of the aforementioned nanoparticles, the nanoparticles are prone to agglomeration, and it is extremely difficult to coat the surface of a single nanoparticle rather than an aggregate of particles. Moreover, when the plasma polymerization method is used to coat nanoparticles, it is also a problem to be solved to selectively "cut" and retain specific functional groups of monomer molecules.
因此针对这两个难题需要寻找改进方法,以提高单一粒子包覆的均匀性,并针对不同应用目的更灵活地裁剪改变包覆膜的表面物理及化学结构。Therefore, to address these two problems, it is necessary to find improved methods to improve the uniformity of single particle coating, and to more flexibly tailor and change the surface physical and chemical structure of the coating film for different application purposes.
发明内容Contents of the invention
针对克服纳米粒子包覆时易产生团聚的问题,以提高单一粒子包覆的均匀性,以及根据不同应用目的更灵活地裁剪包覆膜的表面物理化学结构两个目的,本发明提出一种纳米粒子表面物理化学结构裁剪包覆方法。其作用原理是:首先使纳米粒子带电,粒子产生同性的等离子体鞘电位,利用颗粒同性鞘电位相斥作用,并通过流化或剪切作用施加切向力,使软团聚易于破坏,纳米粒子动态地不断更新暴露于等离子体聚合气氛中,气态单体活性种易于渗入粒子间而产生均匀沉积包覆。同时调控等离子体聚合放电条件,如放电的时间、功率、脉动比等,调控包覆膜的物理化学结构,获得物理化学结构可变的纳米粒子表面,以适用于不同的应用目的。Aiming at overcoming the problem of easy agglomeration when coating nanoparticles, to improve the uniformity of single particle coating, and to more flexibly tailor the surface physical and chemical structure of the coating film according to different application purposes, the present invention proposes a nano Particle surface physicochemical structure tailoring coating method. Its principle of action is: first charge the nanoparticles, the particles generate the same-sex plasma sheath potential, use the repulsion of the same-sex sheath potential of the particles, and apply a tangential force through fluidization or shearing, so that the soft agglomeration is easy to destroy, and the nanoparticles Dynamically and constantly renewed exposure to the plasma polymerization atmosphere, the gaseous monomer active species is easy to penetrate into the particles to produce uniform deposition coating. At the same time, control the plasma polymerization discharge conditions, such as discharge time, power, pulse ratio, etc., control the physical and chemical structure of the coating film, and obtain the surface of nanoparticles with variable physical and chemical structures, so as to be suitable for different application purposes.
本发明纳米粒子表面物理化学结构裁剪包覆方法,包括以下步骤:The nanoparticle surface physicochemical structure cutting coating method of the present invention comprises the following steps:
(1)被包覆纳米粒子预先经高压静电发生器作用,使之带电。可采用市售高压静电发生器,放电时间1-20分钟,电压10-100KV,取出后立即置入等离子体反应器(如图1所示)的多孔分配板上;(1) The coated nanoparticles are pre-charged by a high-voltage electrostatic generator. A commercially available high-voltage electrostatic generator can be used, with a discharge time of 1-20 minutes and a voltage of 10-100KV, and immediately put it into the porous distribution plate of the plasma reactor (as shown in Figure 1) after taking it out;
(2)反应器抽真空至本底真空度≤10Pa,将单体与载气按比例混合成混合气体,通过多孔分配板以一定的速度流向导入等离子体反应器,使粒子处于流化状态,而且通过粒子间静电相斥作用,使软团聚易于通过流化或剪切作用破坏,气态单体原子或基团易于渗入粒子间均匀沉积包覆。单体与载体的混合体积比是1-10∶1-95,控制混合气体流速5-150sccm(每分钟标准立方升),反应器真空度达15-300Pa。(2) The reactor is evacuated to a background vacuum degree of ≤10Pa, and the monomer and the carrier gas are mixed in proportion to form a mixed gas, which flows into the plasma reactor at a certain speed through the porous distribution plate, so that the particles are in a fluidized state, Moreover, through the electrostatic repulsion between particles, the soft agglomeration is easy to be destroyed by fluidization or shearing, and the gaseous monomer atoms or groups are easy to penetrate into the particles for uniform deposition and coating. The mixing volume ratio of the monomer and the carrier is 1-10:1-95, the flow rate of the mixed gas is controlled at 5-150 sccm (standard cubic liter per minute), and the vacuum degree of the reactor reaches 15-300 Pa.
(3)开启脉动射频等离子体发生器与搅拌器。通过电容耦合线圈在反应器内形成放电,使导入的单体放电聚合,并包覆在纳米粒子表面。脉动射频等离子体发生器频率13.56MHz,最大功率600W。反应器可以进行脉动调制,使放电在“开”与“关”之间间歇进行,脉动比(“开”的时间除以“开”和“关”的时间总和)为1-100%,“开”的时间范围为1μs-50ms,等离子体反应器电极为电容耦合式,放电功率2-500W,聚合包覆时间视包覆厚度需要而定,可为0.1-15小时。在反应结束后,包覆后的纳米粒子可在过滤收集器收集或在反应器下部收集。等离子体反应器内的搅拌器是由斜度为0-45°的1-40对的刀形叶片组成,叶片宽0.5-2.0cm,通过电机带动,搅拌速度50-2000转/分,搅拌器安装高度10-50cm,以提高软团聚的破坏程度,更新粒子表面,使其动态分散于等离子体气氛中,达到单一粒子均匀包覆的效果。(3) Turn on the pulsating radio frequency plasma generator and the stirrer. A discharge is formed in the reactor through a capacitive coupling coil, so that the introduced monomer discharge is polymerized and coated on the surface of nanoparticles. Pulse radio frequency plasma generator frequency 13.56MHz, maximum power 600W. The reactor can be pulsatingly modulated so that the discharge is performed intermittently between "on" and "off", and the pulse ratio (the time of "on" divided by the sum of the time of "on" and "off") is 1-100%, " The time range of "on" is 1μs-50ms, the plasma reactor electrode is capacitively coupled, the discharge power is 2-500W, and the polymerization coating time depends on the coating thickness, which can be 0.1-15 hours. After the reaction, the coated nanoparticles can be collected in a filter collector or collected in the lower part of the reactor. The stirrer in the plasma reactor is composed of 1-40 pairs of knife-shaped blades with a slope of 0-45°, the blades are 0.5-2.0cm wide, driven by a motor, and the stirring speed is 50-2000 rpm. The installation height is 10-50cm to increase the degree of destruction of soft agglomerates, renew the particle surface, make it dynamically dispersed in the plasma atmosphere, and achieve the effect of uniform coating of a single particle.
所述单体可为常温常压下或减压后能形成气态的化合物(惰性气体及氧、氮、氢等非聚合沉积类气体除外),可以选自丙氨酸、甘氨酸、赖氨酸,丙烯酰胺,乙烯基乙酸、丙烯酸、甲基丙烯酸甲酯、四氟化碳、六氟丙烯、六甲基二硅氧烷、乙烯、乙炔、甲烷、乙醇、丙酮,四羟乙基钛、四甲氧基硅烷、二乙基锌、四甲基锡或硫酸铜等,载气可为带一定压力的非聚合性气体,如氩、氮、氧、氢、压缩空气等。The monomer can be a compound that can form a gaseous state under normal temperature and pressure or after reduced pressure (except for inert gases and non-polymerizable deposition gases such as oxygen, nitrogen, and hydrogen), which can be selected from alanine, glycine, and lysine, Acrylamide, vinyl acetic acid, acrylic acid, methyl methacrylate, carbon tetrafluoride, hexafluoropropylene, hexamethyldisiloxane, ethylene, acetylene, methane, ethanol, acetone, tetrahydroxyethyltitanium, tetramethyldisiloxane Oxysilane, diethylzinc, tetramethyltin or copper sulfate, etc., the carrier gas can be a non-polymerizable gas with a certain pressure, such as argon, nitrogen, oxygen, hydrogen, compressed air, etc.
等离子体反应器内多孔分配板如图2所示。多孔分配板上的孔的下部直径d1∶孔的上部直径d2=1∶1-5,孔的下部直径的高度∶孔的总高度=1-4∶5,孔面积占板面积的1/10~8/10,d2为1~50mm。多孔分配板上覆盖有孔径50-600目的不锈钢滤网或滤纸。这样安排可使气体分布均匀,因而纳米粒子受到适宜的气体冲力而处于良好的流化状态。The porous distribution plate in the plasma reactor is shown in Figure 2. The lower diameter d 1 of the hole on the porous distribution plate: the upper diameter d 2 of the hole = 1: 1-5, the height of the lower diameter of the hole: the total height of the hole = 1-4: 5, the hole area accounts for 1 of the plate area /10~8/10, d2 is 1~50mm. The porous distribution plate is covered with a stainless steel filter screen or filter paper with a pore size of 50-600 mesh. This arrangement can make the gas distribution uniform, so the nanoparticles are in a good fluidized state under the appropriate gas impulse.
本发明具有下列特点与效果:The present invention has following characteristics and effect:
1、本发明方法在包覆时由于纳米粒子带电,可以利用粒子产生的同性的等离子体鞘电位间的相斥作用,并通过气流流化和剪切作用施加切向力,使软团聚易于破坏,纳米粒子动态地不断更新暴露于等离子体聚合气氛中,气态单体活性种易于渗入粒子间而产生均匀沉积包覆。1. The method of the present invention can use the repulsion between the same-sex plasma sheath potentials produced by the particles because the nanoparticles are charged during coating, and apply a tangential force through the fluidization and shearing of the airflow to make the soft agglomeration easy to destroy , Nanoparticles are dynamically updated and exposed to the plasma polymerization atmosphere, and the gaseous monomer active species is easy to penetrate into the particles to produce uniform deposition coating.
2、将射频等离子体进行脉动调制,用于单体的聚合,可较大程度地提高聚合包覆膜中含氧、含氮、含硫等官能团的保留率,调控包覆粒子与基体聚合物的相容性。也可包覆粒子表面具有可进一步反应的官能团。克服射频连续波等离子体包覆膜常见的不溶不熔、高度交联的缺陷,调控包覆膜的化学结构,从而形成化学结构可裁剪控制的纳米粒子表面。2. The radio frequency plasma is pulsated and used for the polymerization of monomers, which can greatly improve the retention rate of oxygen-containing, nitrogen-containing, sulfur-containing and other functional groups in the polymer coating film, and control the coating particles and the matrix polymer. compatibility. It is also possible to coat the particle surface with functional groups that can be further reacted. Overcome the insoluble, infusible, and highly crosslinked defects of radio frequency continuous wave plasma coatings, and regulate the chemical structure of the coating to form a nanoparticle surface that can be tailored to control the chemical structure.
3、控制调节脉动射频等离子体条件,如功率、脉动比、流速、单体配比、时间等,可调节控制包覆层厚度、表面拓扑结构,改变粒子表面物理结构。从而改变包覆粒子的流动性、比重、与基体材料的结合紧密程度、吸附性等。这样,通过包膜的空间物理位阻,可以阻止纳米粒子团聚成较大的颗粒,通过化学相容性及包膜的物理粗糙度等,增进与基体聚合物的分散性,降低纳米粒子的团聚性,以体现小尺寸给纳米粒子带来的特殊效应等。3. Control and adjust the pulsating radio frequency plasma conditions, such as power, pulsation ratio, flow rate, monomer ratio, time, etc., can adjust and control the thickness of the coating layer, surface topology, and change the physical structure of the particle surface. Thus, the fluidity, specific gravity, tightness of combination with matrix material, adsorption, etc. of the coated particles can be changed. In this way, through the steric physical hindrance of the coating, the nanoparticles can be prevented from agglomerating into larger particles, and the dispersion with the matrix polymer can be improved through the chemical compatibility and the physical roughness of the coating, so as to reduce the agglomeration of nanoparticles. properties, in order to reflect the special effects brought by small size to nanoparticles, etc.
4、包覆反应在常温干态进行,可适用于溶解性及非溶解性纳米粒子的包覆,以及对温度敏感的粒子的包覆。并且克服溶剂重复分离等操作,对环境污染小,包覆工艺相对简单。4. The coating reaction is carried out in a dry state at room temperature, which is applicable to the coating of soluble and non-soluble nanoparticles, as well as the coating of temperature-sensitive particles. In addition, it overcomes operations such as repeated separation of solvents, has little environmental pollution, and the coating process is relatively simple.
5、包覆单体选择范围广,可进行有机、无机、金属薄膜的包覆,用于各类纳米复合粒子及纳米/聚合物复合材料、纳米/金属复合材料等的研制。也可用于各类纳米复合颗粒的研制等,形成无机/有机、无机/金属、金属/有机、无机/金属/有机等纳米复合粒子。5. A wide range of coating monomers can be selected, which can be used for coating organic, inorganic, and metal films, and is used for the development of various nanocomposite particles, nano/polymer composite materials, nano/metal composite materials, etc. It can also be used in the development of various nanocomposite particles to form inorganic/organic, inorganic/metal, metal/organic, inorganic/metal/organic and other nanocomposite particles.
附图说明Description of drawings
图1是等离子体包覆反应器装置示意图。Figure 1 is a schematic diagram of a plasma coating reactor device.
图2是等离子体反应器内的多孔分配板示意图Figure 2 is a schematic diagram of the porous distribution plate in the plasma reactor
其中d1孔的下部直径 h1孔下部直径的高度where d1 is the lower diameter of the hole h1 is the height of the lower diameter of the hole
d2孔的上部直径 h2孔的总高度。d 2 the upper diameter of the hole h 2 the total height of the hole.
图3是等离子体丙烯酸包覆前后TiO2纳米粒子的HRTEM图Figure 3 is the HRTEM images of TiO nanoparticles before and after plasma acrylic coating
其中a未包覆 b等离子体包覆后。 a is uncoated b after plasma coating.
图4是等离子体经丙烯酸包覆前后TiO2纳米粒子的EDS谱图Figure 4 is the EDS spectrum of TiO2 nanoparticles before and after plasma coating with acrylic acid
其中a未包覆 b等离子体包覆后。 a is uncoated b after plasma coating.
图5是等离子体六甲基二硅氧烷包覆的Cr2O3纳米粒子的HRTEM图。Figure 5 is an HRTEM image of plasmonic hexamethyldisiloxane coated Cr2O3 nanoparticles.
图6是等离子体六甲基二硅氧烷膜的AFM图Figure 6 is an AFM image of a plasmonic hexamethyldisiloxane film
其中a脉动比3%,脉动“开”的时间为15ms,放电功率3WAmong them, the pulsation ratio of a is 3%, the pulsation "on" time is 15ms, and the discharge power is 3W
b连续波,放电功率30W。b Continuous wave, discharge power 30W.
图7是等离子体六甲基二硅氧烷膜的AFM剖面粗糙度比较图Figure 7 is a comparison chart of the AFM cross-sectional roughness of the plasma hexamethyldisiloxane film
其中a脉动比3%,脉动“开”的时间为15ms,放电功率3WAmong them, the pulsation ratio of a is 3%, the pulsation "on" time is 15ms, and the discharge power is 3W
b连续波,放电功率30W。b Continuous wave, discharge power 30W.
图8是不同等子体包覆条件下的TiO2纳米粒子的红外光谱图Figure 8 is the infrared spectrum of TiO2 nanoparticles under different isoplasmic coating conditions
其中a未包覆where a is not covered
b丙烯酸包覆,脉动比2%b Acrylic coating,
c丙烯酸包覆,脉动比40%。c Acrylic coating, pulsation ratio 40%.
图9是不同包覆条件对TiO2纳米粒子紫外吸光性的影响。Figure 9 is the effect of different coating conditions on the UV absorbance of TiO 2 nanoparticles.
具体实施方式Detailed ways
实施例1 纳米粒子TiO2的等离子体聚合均匀包覆Example 1 Uniform Coating of Nanoparticle TiO2 by Plasma Polymerization
采用图1所示的等离子体包覆反应器装置进行包覆试验。首先将包覆对象TiO纳米粒子,平均粒径30nm左右,预先经50KV高压静电发生器作用5分钟,使之带电,取出后立即置入等离子体反应器6下部的多孔分配板3(详细结构参见图2)上。反应器6由真空系统7抽真空至本底真空度5Pa。将单体丙烯酸与载气氩气分别通过流量计1计量,按体积比为1∶50,在气体混合器2中均匀混合后,通过多孔分配板3,以10sccm的流速导入等离子体反应器6,使粒子处于流化状态,真空度下降至150Pa。开启脉动射频等离子体发生器5与搅拌器4。发生器5通过电容耦合线圈在反应器6内形成放电,使导入的单体放电聚合,并包覆在纳米粒子表面。脉动射频等离子体发生器5频率13.56MHz,最大功率600W。反应器6进行脉动调制,放电的脉动比100%,“开”的时间为1ms,放电时间为4小时,放电功率为20W。搅拌器4是由斜度为30°的30对刀形叶片组成,叶片宽1cm,搅拌速度1000转/分,搅拌器安装高度20cm,以提高软团聚的破坏程度,更新粒子表面使其动态分散于等离子体气氛中,达到单一粒子均匀包覆的效果。在反应结束后,包覆后粒子在过滤收集器8收集或在反应器6下部收集。The coating test was carried out using the plasma coating reactor apparatus shown in Fig. 1 . First, the TiO nanoparticles to be coated, with an average particle diameter of about 30nm, are pre-acted by a 50KV high-voltage electrostatic generator for 5 minutes to make it charged. After taking it out, immediately put it into the
包覆后样品经高分辨透射电镜(HRTEM)检测(图3),未包覆的TiO2纳米粒子可见其晶体的层状结构(图3中a),但外表面未见半透明的无定形有机包覆层或其它层状晶体结构的包覆层,而经丙烯酸等离子体聚合包覆的TiO2除可见其晶体的层状结构外,外圈可见一层半透明的无定形丙烯酸等离子体聚合物有机包覆层,均匀包覆在TiO2层状晶体外圈,厚度约为5nm左右(图3中b)。X光能量散射谱(EDS)表明,包覆前钛峰强度较高(图4中a),包覆后钛峰强度下降为零(图4中b),氧峰、碳峰强度上升,说明包覆的等离子体聚丙烯酸薄膜相当有效且均匀,所以钛元素不再被检测到。After the coating, the sample was detected by high-resolution transmission electron microscopy (HRTEM) (Figure 3). The uncoated TiO 2 nanoparticles can be seen in its crystal layered structure (a in Figure 3), but there is no translucent amorphous shape on the outer surface. Organic coating layer or coating layer of other layered crystal structure, and TiO 2 coated by acrylic acid plasma polymerization can be seen in addition to its crystal layered structure, and a layer of translucent amorphous acrylic plasma polymerization can be seen on the outer ring The organic coating layer is evenly coated on the outer ring of TiO 2 layered crystals, with a thickness of about 5nm (b in Figure 3). X-ray Energy Scattering Spectroscopy (EDS) showed that the titanium peak intensity was higher before coating (a in Figure 4), and the titanium peak intensity decreased to zero after coating (Figure 4 b), and the oxygen peak and carbon peak intensity increased, indicating that The coated plasma polyacrylic film is quite effective and homogeneous, so that titanium element is no longer detected.
实施例2 Cr2O3纳米粒子等离子体包覆条件影响包覆厚度的试验Example 2 Cr 2 O 3 nanoparticle plasma coating conditions affect the test of coating thickness
采用图1所示的等离子体包覆反应器装置,操作步骤参照实施例1。The plasma coating reactor device shown in FIG. 1 is used, and the operation steps refer to Example 1.
以Cr2O3纳米粒子为包覆对象,平均粒径150nm,经20KV高压静电发生器作用1分钟使之带电,立即置入等离子体反应器6中,抽真空至本底真空度4Pa,通入六甲基二硅氧烷与氮的混合气体,两种气体的体积比为10∶50,流速60sccm,真空度下降至200Pa。开启等离子体发生器5与搅拌器4,控制放电的功率为40W,放电时间为8小时,放电的脉动比50%,脉动“开”的时间为2ms,搅拌速度500转/分。Take Cr 2 O 3 nanoparticles as the coating object, with an average particle size of 150nm, and charge it through a 20KV high-voltage electrostatic generator for 1 minute, and immediately put it into the plasma reactor 6, and vacuumize it to the background vacuum degree of 4Pa. Inject the mixed gas of hexamethyldisiloxane and nitrogen, the volume ratio of the two gases is 10:50, the flow rate is 60 sccm, and the vacuum degree drops to 200 Pa. Turn on the
包覆后样品经高分辨透射电镜(HRTEM)检测(见图5),结果表明,粒子表面都均匀包覆一层厚度约为25nm左右的等离子体聚合的六甲基二硅氧烷薄膜。After coating, the sample was detected by high-resolution transmission electron microscopy (HRTEM) (see Figure 5), and the results showed that the surface of the particles was uniformly coated with a plasma-polymerized hexamethyldisiloxane film with a thickness of about 25 nm.
实施例3 脉动射频等离子体包覆条件影响包覆膜表面粗糙度的试验Example 3 The test of the effect of pulsating radio frequency plasma coating conditions on the surface roughness of the coating film
采用图1所示的等离子体包覆反应器装置。The plasma coating reactor setup shown in Fig. 1 was used.
为了观察脉动射频等离子体包覆条件与包覆膜表面粗糙度的关系,选择平整的玻璃片为涂层对象,清洗干净后,置入等离子体反应器6中,抽真空至本底真空度4Pa,通入六甲基二硅氧烷与氩气的混合气体,两种气体的体积比为10∶90,流速10sccm,使真空度下降至30Pa。开启等离子体发生器5,放电聚合。放电时间为1小时,聚合结束,取出样品做原子力显微镜(AFM)分析,所得样品的原子力显微镜图见图6。图6中a放电功率为3w、脉动比3%、脉动“开”的时间为15ms,图6中b放电功率为30w,连续波。亮度越大,代表平面高度越高。图7中a和b为图6中a和b样品的剖面图。曲线高低代表膜剖面的起伏。从该AFM的检测结果可知,低脉动比、低功率的条件下(图6中a、图7中a),包膜为纳米级的颗粒膜组成,包膜起伏粗糙度为数纳米;连续波高功率情况下(图6中b、图7中b),包膜为微米级的大颗粒膜组成,包膜起伏粗糙度为数微米。改变包膜条件,可以有效改变包膜的粗糙度。In order to observe the relationship between the pulsating radio frequency plasma coating conditions and the surface roughness of the coating film, a flat glass sheet is selected as the coating object. After cleaning, it is placed in the plasma reactor 6 and vacuumed to a background vacuum of 4Pa. , into a mixed gas of hexamethyldisiloxane and argon, the volume ratio of the two gases is 10:90, the flow rate is 10 sccm, and the vacuum is reduced to 30 Pa. Turn on the
实施例4 包覆条件影响TiO2纳米粒子表面化学结构的试验Example 4 Coating Conditions Affect TiO Nanoparticle Surface Chemical Structure Test
采用图1所示的等离子体包覆反应器装置,操作步骤参照实施例1。The plasma coating reactor device shown in FIG. 1 is used, and the operation steps refer to Example 1.
采用图1所示的等离子体包覆反应器装置,操作步骤参照实施例1。The plasma coating reactor device shown in FIG. 1 is used, and the operation steps refer to Example 1.
包覆对象TiO2纳米粒子,平均粒径30nm左右,TiO2纳米粒子预先经35KV高压静电发生器作用3分钟,使之带电,立即置入等离子体反应器6中,抽真空至本底真空度3Pa,通入丙烯酸与氩气的混合气体,两种气体的体积比为5∶50,流速35sccm,使真空度下降至85Pa。开启等离子体发生器5与搅拌器4,控制放电的功率为20w,放电时间为2小时,搅拌速度1000转/分,放电的脉动比为2%、40%。Coating target TiO 2 nanoparticles, with an average particle size of about 30nm, TiO 2 nanoparticles are pre-acted by a 35KV high-voltage electrostatic generator for 3 minutes to make them charged, and immediately placed in the plasma reactor 6, and vacuumed to the background vacuum 3Pa, a mixed gas of acrylic acid and argon is introduced, the volume ratio of the two gases is 5:50, the flow rate is 35 sccm, and the vacuum degree is reduced to 85Pa. Turn on the
包覆处理后的TiO2纳米粒子样品与KBr粉按照一定比例共混碾磨压片,经Nicolet公司生产的NEXUS-670型傅里叶光谱仪测定包覆TiO2纳米粒子的红外光谱,以测试包覆TiO2纳米粒子的化学结构如图8所示。图8中(a)为未经包覆的TiO2纳米粒子的红外光谱图,图8中(b)和(c)分别为脉动比2%、40%时包覆处理的TiO2纳米粒子的红外光谱图。由于包覆层薄,红外透射谱测试的结构也不仅仅反映表面,所以图8中(a)(b)(c)可见,400-700cm-1范围都有很强的吸收峰,这是Ti-O-Ti键的特征吸收峰,在3300cm-1附近都有较宽的由于水的吸附等引起的-OH的伸缩振动峰。1631cm-1附近的吸收峰也是由于表面羟基化产生的-OH的伸缩振动峰。经脉动比2%的丙烯酸等离子体包覆处理之后,在1433cm-1附近出现了一新的肩峰,脉动比40%时,这一肩峰发展成为一新吸收峰。由于这一位置的吸收与CH3-O-或CH2-O-等基团中CH变形振动有关,该峰相对强度的高低,说明不同脉动比条件下,包覆膜中类似CH3-O-或CH2-O的酯基的含量不一。不同包覆条件,可以改变包膜化学结构中基团的含量,甚至种类。The coated TiO2 nanoparticle sample and KBr powder were blended and ground into tablets according to a certain ratio, and the infrared spectrum of the coated TiO2 nanoparticle was measured by the NEXUS-670 Fourier spectrometer produced by Nicolet Company to test the coating. The chemical structure of the coated TiO2 nanoparticles is shown in Fig. 8. Among Fig. 8 (a) is the infrared spectrogram of uncoated TiO2nanoparticle , among Fig. 8 (b) and (c) are the TiO2 nanoparticle of coating process when
实施例5 包覆条件影响TiO2纳米粒子紫外吸光性能的试验Example 5 Coating Conditions Affect TiO 2 Experiments on the Ultraviolet Absorption Properties of Nanoparticles
采用图1所示的等离子体包覆反应器装置,操作步骤参照实施例1。The plasma coating reactor device shown in FIG. 1 is used, and the operation steps refer to Example 1.
包覆对象TiO2纳米粒子,平均粒径30nm左右,TiO2纳米粒子经100KV高压静电发生器作用1分钟,立即置入等离子反应器6中。抽真空至本底真空度3Pa,通入六甲基二硅氧烷与氩气的混合气体,两种气体的体积比为5∶95,流速50sccm,使真空度下降至150Pa。开启等离子体发生器5与搅拌器4,控制放电的功率为60w,放电时间为4小时,搅拌速度2000转/分,放电的脉动比为5%、15%、40%。The TiO 2 nanoparticles to be coated have an average particle size of about 30nm. The TiO 2 nanoparticles are subjected to a 100KV high-voltage electrostatic generator for 1 minute, and then placed into the plasma reactor 6 immediately. Vacuumize to the background vacuum degree of 3Pa, and pass a mixed gas of hexamethyldisiloxane and argon, the volume ratio of the two gases is 5:95, and the flow rate is 50 sccm, so that the vacuum degree drops to 150Pa. Turn on the
处理后样品经乙二醇配成0.015%的悬浮液,倒入0.5cm的石英比色皿中,用752分光光度计测其在紫外一可见光的吸收值。所得结果如图9所示。不同的脉动比下,由于包覆层的物理化学结构不同,包覆的TiO2纳米粒子在乙二醇溶液中吸光性就不同。因为分散性好,团聚粒径小,对紫外光的吸收性好。所以吸光性的好坏也代表了分散性的好坏。从图9可见,尽管在不同脉动比条件下包覆的TiO2纳米粒子在乙二醇溶液中吸光性不同,但都比未包覆TiO2纳米粒子的乙二醇溶液的吸光性好,也说明包覆的TiO2纳米粒子在乙二醇溶液中分散性比未包覆TiO2纳米粒子的分散性好。After treatment, the sample was made into a 0.015% suspension with ethylene glycol, poured into a 0.5 cm quartz cuvette, and measured its absorption value in ultraviolet-visible light with a 752 spectrophotometer. The results obtained are shown in Fig. 9 . Under different pulsation ratios, due to the different physical and chemical structures of the coating layer, the light absorption of the coated TiO 2 nanoparticles in ethylene glycol solution is different. Because of good dispersion, small aggregate particle size, and good absorption of ultraviolet light. Therefore, the quality of light absorption also represents the quality of dispersion. It can be seen from Figure 9 that although the coated TiO2 nanoparticles have different absorbances in ethylene glycol solutions under different pulsation ratio conditions, they are all better than uncoated TiO2 nanoparticles. It shows that the dispersibility of coated TiO 2 nanoparticles in ethylene glycol solution is better than that of uncoated TiO 2 nanoparticles.
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