声化学反应器设计理论进展

论述了近年来连续声场中声化学产额与声强、超声辐照时间之间的关系,反应器的类型(PFR和CSTR)与反应器中物料衡算方程,超声空化效应峰值(空化峰)对反应器设计的作用,空化效应动力学对声化学反应的影响以及换能器与反应溶液的电-声耦合关系等声化学反应器设计理论研究方面的若干进展,并对未来的研究作了简要展望。     

开放式声化学反应体系中的反应动力学

采用气液传质的双膜理论建立了开放体系中声化学反应的动力学模型，同时用声源频率为500 kHz，声强为3 W·cm^-2的超声波在开放式声化学反应器内引发被空气饱和溶解的KI纯水溶液中的声化学反应，并检测反应过程中溶液的电导率，pH值改变及KI溶液中I₂的析出量，结果表明，它们与超声辐照时间之间呈线性关系，与理论模型吻合。     

声化学降解染料结晶紫的研究

采用频率为20 kHz的超声波降解阳离子染料结晶紫(CV)溶液,考察了溶液初始浓度、pH值、声能强度、时间、温度等因素对染料声化学降解过程的影响.实验结果表明,溶液初始浓度为30 mg/L、pH=8.0、声强=47.5 W/cm2、超声辐照50 m in,CV的脱色率达97.8%;CV的超声降解过程以高温热解反应为主,服从动力学一级反应;当超声/H2O2、超声/镁联合作用时,二者产生协同效应,溶液中产生大量OH自由基,强化了CV的声化学脱色和降解过程.     

超声化学在生物医学中应用的研究进展

超声是一类频率超过人类听力上限的机械波,具有高能和高穿透性的特点,能穿透生物体软组织的阻碍,在其内部诱导发生化学反应.近年来,超声化学手段越来越多地被应用于生物医学的研究当中,并为生物医学的发展提供了新的着力点.本文从三个方面,即超声的机械化学作用、声敏剂辅助的超声化学和超声的空化效应,总结并综述了超声化学在生物医学领域应用的研究进展.     

声化学反应器基础理论的研究进展

论述了声化学反应器的基础理论,主要涉及反应器中的声化学反应动力学、空化声场中空化泡的分布和检测方法,以及声化学反应器的放大理论,包括反应效率和经济性估算。     

超声MnO2联用降解丁基罗丹明B染料

采用超声MnO2体系降解丁基罗丹明B染料,考察了pH值、声强、MnO2投加量等因素对染料降解过程的影响。实验结果表明,溶液pH=3.0,MnO2投加量为1.5g/L,声强=40.7W/cm2,超声辐照10mg/L的罗丹明B溶液48m in,染料的脱色率为98.73%;超声和MnO2的协同效应在酸性条件下较为明显,溶液中产生大量.OH强化了对染料的声化学脱色和降解过程;丁基罗丹明B的超声降解过程以自由基的氧化反应为主,服从动力学一级反应。     

超声技术在纳米材料制备中的应用

对超声技术在纳米材料制备中的应用与研究进展作了比较全面的综述,着重介绍了与超声有关的纳米材料制备方法,包括雪声雾化－热分解法,金属有机物超声热分解法,化学沉淀法和声电化学法,并就这些方法中声化作用的机理,特点和影响因素进行了讨论。     

声化学反应器在脱除SO2过程中的应用

通过对常用的声化学设备使用情况的分析,根据超声解吸柠檬酸钠溶液中二氧化硫过程的特点,自行设计了一套用于气液传质的多参数可控的声化学反应器,频率为40kHz,功率为0～300W。随后使用该反应器对脱除柠檬酸钠溶液中二氧化硫的过程进行了研究。结果表明,超声波能够较大地促进二氧化硫的脱除,在超声场下工作5h,二氧化硫的脱除率比无超声时高25%;超声场下,二氧化硫脱除率在50℃时达到最大值;在相同搅拌强度下,有超声波比无超声波时二氧化硫脱除率均大25%。     

声化学及其应用

人们对电、光、磁、辐射等多种形式的能量与化学反应的关系及其变化规律进行了广泛的研究,形成了相应的电化学、光化学、磁化学和辐射化学等学科。近年来,人们对于声作为一种新的能量形式变革化学反应发生了浓厚的兴趣,因为声化学效应及其规律具有广泛的实际应用,它所获得的信息和成果不断地丰富着化学学科,促进了声学和化学的交叉渗透,导致一门崭新的学科——声化学的诞生。     

几种简易安全的声化学消解器的制作及其应用

试样的分 (消 )解工作是分析工作的重要步骤之一。传统的水热消解法加热时间长 ,试剂耗量多 ,环境污染严重 ,已不适应现代分析工作的要求。新近兴起的微波消化技术虽能大大缩短样品的分解时间 ,但仍然存在许多不安全的因素而难于推广使用。本文推出几种简易安全的声化学消解装置 ,将其应用于低浓度、难消解的有机物和脆性固体无机物的预处理 ,结果表明消化效果较好。1　声化学消解原理超声波作为一种波动形式 ,早已广泛用于军事探测和信息传递。作为一种能量形式通过介质时 (当声强超过某一定值时 ) ,液体中的微泡会在超声场共振作用下产生…     

Correlation in spatial intensity distribution between volumetric bubble oscillations and sonochemiluminescence in a multibubble system

The correlation in spatial intensity distribution between volumetric oscillation of multibubble and sonochemiluminescence in an ultrasonic standing-wave field is investigated through the measurements of scattered light from bubbles by changing the measuring position in the direction of sound propagation and sonochemiluminescence with luminol. When a thin light sheet, finer than half the wavelength of sound, is introduced into the cavitation bubbles at the anti-node of the sound pressure, the scattered light intensity oscillates temporally. The peak-to-peak light intensity corresponds to the number of the bubbles which contribute to the sonochemical reaction because the radius for oscillating bubbles at pressure antinode is restrictive in a certain range due to the shape instability and the action of Bjerknes force that expels from anti-node bubbles larger than the resonant size. The experimental results show that at the side near the water surface, the peak-to-peak light intensity is larger in comparison with the intensity near the sound source, and this tendency becomes apparent at higher input power. These light scattering results correspond with the spatial intensity distribution of the sonochemiluminescence with luminol. Therefore, it is interpreted that most of the cavitation bubbles contributing to the sonochemical reactions in the standing wave field exist near liquid surface. Present method of light scattering in reference with the image of the sonochemiluminescence is promising for evaluating spatial distribution of violently oscillating cavitation bubbles effective for sonochemical reactions.     

The effect of high intensity ultrasound on the synthesis of some polyurethanes

High intensity ultrasound has been applied to the preparation of polyurethanes from a number of diisocyanates and diols. In all cases, the sonochemical reactions proceeded faster in the early stages and led to higher molecular weight polymers. The effect of changing the ultrasound intensity is discussed and some speculation as to the mechanism of the reaction enhancement is given.     

Enhancement of sonochemical reaction rate by addition of micrometer-sized air bubbles

The sonochemical reaction rate has been enhanced by the introduction of tiny air bubbles. The bubbles including micrometer-sized ones are produced by method of atomization and are introduced into aqueous luminol solution under 141-kHz sonication in order to investigate the enhancement of sonochemical reaction rate by introduction of tiny bubbles through the intensity measurement of sonochemiluminescence (SCL). It is shown that the introduction of tiny bubbles under sonication accomplishes the large SCL intensity compared to the cases of sonication only and liquid flow under sonication. It is also shown that it is important to adjust the configuration of tiny-bubble addition to the sound field. Through the investigations on the intensity and the spatial pattern of luminol-SCL, it has been clarified that tiny bubbles added into the sonicated liquid not only cause the liquid flow but also increase the number of collapsing bubbles active for sonochemical reaction. It is also shown that the tiny-bubble addition enhances the reaction rate of KI oxidation under sonication. Therefore, the present method of introduction of tiny bubbles is effective for enhancement of sonochemical reaction rate.     

Correlation between acoustic cavitation noise and yield enhancement of sonochemical reaction by particle addition

The mechanism of the effect of particle addition on sonochemical reaction is studied through the measurements of frequency spectrum of sound intensity for evaluating the cavitation noise and the absorbance for the liberation of iodine from an aqueous solution of KI as an index of oxidation reaction by ultrasonic irradiation in the presence or absence of alumina particles. As it is expected that both the acoustic noise and a rise in temperature in the liquid irradiated by intense ultrasound will increase with the number of collapsing bubbles, these are supposed to be the best tools for evaluating the relative number of bubbles. In the present investigation, it has been shown that the addition of particles with appropriate amount and size results in an increase in the absorbance when both the acoustic noise and the rise in the liquid temperature due to cavitation bubbles also increase. This suggests that the enhancement in the yield of sonochemical reaction by appropriate particle addition comes from an increase in the number of cavitation bubbles. The existence of particle in liquid provides a nucleation site for cavitation bubble due to its surface roughness, leading to the decrease in the cavitation threshold responsible for the increase in the number of bubbles when the liquid is irradiated by ultrasound. Thus, from the present investigation, it is clarified that the particle addition has a potential to enhance the yield in the sonochemical reaction.     

Ultrasonic cleavage of thioethers

The rates of DPPH (diphenylpicrylhydrazyl) trapping and the sonolytical products obtained during the sonolysis of thioethers at normal and low temperature are reported. CS2, lower sulfides, thiophene, and sulfurized species are the common products during the ultrasonic irradiations. Hydrocarbons are also obtained during the sonolysis of diallyl sulfide, diethyl disulfide, and dipropyl disulfide. Furthermore, aldehydes are obtained as oxidized species; SO2 is found at 208 K. The principal sonochemical process appears to be the cleavage of C-S or S-S bond with secondary combinations and rearrangements. DPPH has been used to probe the sonolytical potential of thioethers. The results show a good correlation between the rates of DPPH trapping and the vapor pressures of thioethers. In conclusion, a lower vapor pressure results in a higher sonolytical rate. The sonochemical behaviors of thioethers have strong qualitative similarities to the pyrolysis.     

Ultrasonic characterization of proteins and blood cells

Ultrasound changes its intensity and speed when propagating through a liquid or a suspension containing particles. In addition it generates a weak electric signal by altering the motion of ions and charged particles. Hence acoustic and electroacoustic measurements provide information about the properties of suspended particles and molecules. Here we present both acoustic and electroacoustic results on blood suspensions and protein solutions, relevant to life sciences. For blood cells a strong increase in acoustic attenuation with volume fraction is found, from which the speed of sound in an erythrocyte is found to be about 1900 m/s, assuming the attenuation is due to scattering only. A similar value of 1700 m/s is found from the increase in sound speed of the dispersion with concentration. Electroacoustic measurements on bovine serum albumin (BSA) yield a charge of about seven elementary charges per BSA molecule. These results show the power and usefulness of acoustic and electroacoustic measurement techniques for biological systems.     

Mist separation and sonochemiluminescence under pulsed ultrasound

Differences in the amount of water-mist separation and the intensity of luminol chemiluminescence for pulsed and continuous-wave (CW) ultrasound at 135 kHz have been investigated. The amount of mist generated is estimated using the cooling rate of a copper plate sprayed with the mist. For pulsed operation with an appropriate duty cycle, the cooling rate and the cooling rate per input power to the transducer are higher by 4 and 12 times compared to CW operation, respectively. This is due to the amplitude of the pulsed ultrasound being higher than that for CW ultrasound. Relatively low power pulsed operation can successfully produce both a higher sonochemiluminescence (SCL) intensity and cooling rate than those for CW ultrasound. The sonochemical reaction for pulsed ultrasound occurs at the same input power threshold as that for mist separation, whereas for CW ultrasound, the former threshold is lower than the latter. A higher number of large bubbles is produced with CW ultrasound than that with pulsed ultrasound. To achieve a sound pressure amplitude sufficient for mist separation near the surface of a liquid, it is necessary to expel these bubbles by changing the sound field from resonant standing waves to progressive waves that give rise to capillary waves on the liquid surface.     

Ultrasonic characterization of proteins and blood cells

Ultrasound changes its intensity and speed when propagating through a liquid or a suspension containing particles. In addition it generates a weak electric signal by altering the motion of ions and charged particles. Hence acoustic and electroacoustic measurements provide information about the properties of suspended particles and molecules. Here we present both acoustic and electroacoustic results on blood suspensions and protein solutions, relevant to life sciences. For blood cells a strong increase in acoustic attenuation with volume fraction is found, from which the speed of sound in an erythrocyte is found to be about 1900 m/s, assuming the attenuation is due to scattering only. A similar value of 1700 m/s is found from the increase in sound speed of the dispersion with concentration. Electroacoustic measurements on bovine serum albumin (BSA) yield a charge of about seven elementary charges per BSA molecule. These results show the power and usefulness of acoustic and electroacoustic measurement techniques for biological systems.     

Demulsification of Gas Oil/Water Emulsion via High-Intensity Ultrasonic Standing Wave

High-intensity ultrasonic standing wave field was established in a horizontal direction and its effect on “gas oil” in “water” emulsion separation rate was studied. Also, effects of four parameters on emulsion instability behavior were investigated: ultrasound irradiation time (5–30 min), emulsion position in ultrasound field (17–37 cm), ultrasound input intensity (20, 45, and 75%) and dispersed phase concentration (0.5, 2, and 10%). Emulsion light absorbance, droplet diameter and distribution were measured to analyze separation efficiency. The optimum states were 10% oil in water emulsion treated at 17 cm distance from ultrasound source under 30 minutes irradiation time and 20% sound intensity.     

甲烷在飞秒强激光场中的解离

用波长为800 nm，脉宽为160 fs，强度范围为7.6×1013～1.4×1014 W•cm－2的强激光使甲烷分子解离，并用质谱仪检测产生的离子.母体离子在较低的激光强度（7.6×1013 W•cm－2）下出现;当激光强度增加到8.0×1013 W•cm－2时，开始出现；CH2＋、CH＋和C＋离子出现的阈值分别为1.0×1014 W•cm－2、1.4×1014 W•cm－2和1.4×1014 W•cm－2.这些现象表明甲烷的解离是一个顺序过程.质谱图中没有多电荷离子，因此排除了发生库仑爆炸的可能.以线偏振激光作用于甲烷，只有H＋离子有各向异性的角度分布，暗示分子中的化学键是被激光外场拉断的，且初级产物离子H＋是沿着激光电场的方向飞出.提出的准双原子分子模型较好地解释了实验结果.