高压脉冲等离子体降解水中苯酚的实验研究

对高压脉冲放电等离子体技术降解水中有机污染物苯酚进行了实验研究,观察了脉冲成形电容、脉冲峰值电压、脉冲频率、放电电极直径、放电距离、苯酚的人口质量浓度等因素对苯酚降解率的影响;实验结果表明脉冲成形电容有一最佳值;降解率随脉冲峰值电压、脉冲频率增大而升高,随放电电极直径和放电距离的减小而增大,随苯酚人口质量浓度增大而增大。     

输油管道静电放电形式及危害防护研究

油品管输过程中产生的静电是影响油料安全运输的主要危险源之一。总结了输油管道静电起电的宏观和微观过程及影响管道带电的因素,根据各种静电放电类型的发生条件以及金属、绝缘管道(软管、胶管)自身特性,分析得出金属管道的放电形式主要是电晕放电和火花放电,而绝缘管道的放电形式主要是火花放电和刷形放电。针对金属管道和绝缘管道输油作业中可能发生的静电危害事故,从油品进入管道前、管道中及其他如温湿度控制等3方面提出了一系列防护措施。     

UV-Fenton 体系氧化降解苯酚废水反应动力学研究

利用UV-Fenton高级氧化技术对苯酚废水进行了处理研究.通过半衰期法对苯酚的反应级数进行了探讨,确定其在UV-Fenton体系降解过程中的表观反应级数为3/2,并初步建立了苯酚UV-Fenton降解的动力学模型,并从反应速率系数着手探讨了污染物初始浓度、双氧水加入量、亚铁离子浓度及pH值对反应降解速率的影响.     

波茨坦短芽孢杆菌降解4-氯酚和苯酚的特性

考察了波茨坦短芽孢杆菌对4-氯酚的降解特性及4-氯酚与苯酚在双底物体系中的相互作用。结果表明,波茨坦短芽孢杆菌能以4-氯酚为唯一碳源和能源,完全降解200 mg/L、250 mg/L及300 mg/L的4-氯酚所需时间分别为48 h、63 h和84 h,但该菌无法降解350 mg/L的4-氯酚,表明较高浓度的4-氯酚对细胞生长有较强的抑制作用。酶活分析表明,4-氯酚可诱导波茨坦短芽孢杆菌合成氯代邻苯二酚1,2-加氧酶并通过邻位裂解途径降解。细胞生长动力学过程符合Haldane方程,动力学参数为细胞最大比生长速μmax=0.145 h~(-1),半饱和系数KS=30.45 mg/L,底物抑制系数Ki=127.62 mg/L,决定系数R~2=0.98。在4-氯酚和苯酚双底物降解过程中,4-氯酚的存在会抑制苯酚的降解,当4-氯酚初始质量浓度为40 mg/L时,1 400 mg/L苯酚被完全降解耗时更长,菌体优先利用苯酚作为碳源和能源,苯酚被完全降解后大部分4-氯酚才开始被降解;苯酚对4-氯酚降解的影响体现为低浓度促进和高浓度抑制,苯酚促进时质量浓度为100~300 mg/L,而苯酚质量浓度高于300 mg/L会产生抑制作用,当苯酚初始质量浓度为200 mg/L时4-氯酚降解速率最大。采用Abuhamed动力学方程可以准确描述4-氯酚/苯酚双底物降解体系中细胞生长过程,苯酚对4-氯酚降解的抑制程度I_(1,2)=1.47,4-氯酚对苯酚降解的抑制程度I_(2,1)=2.56,决定系数R~2=0.95。研究表明,4-氯酚对苯酚降解的抑制作用大于苯酚对4-氯酚。     

漆酶介体系统对蒽与苯酚共存体系的降解研究

以2,2-联氮-二(3-乙基-苯并噻唑-6-磺酸)二铵盐(ABTS)为介体,研究了漆酶/ABTS介体系统对蒽与苯酚共存体系的降解效果,并考察了不同苯酚浓度对共存体系中蒽降解效果的影响。同时,分析了漆酶/ABTS介体系统对共存体系的作用机理。结果表明,苯酚的引入会抑制蒽的去除,且随着苯酚浓度的增大,蒽降解被抑制地更明显,而蒽对苯酚的降解影响可以忽略不计;蒽体系和蒽与苯酚共存体系中蒽的氧化降解过程均符合一级动力学规律。     

五氯苯酚的降解研究进展

综述了近年来我国在五氯苯酚(PCP)降解研究中取得的进展,并对五氯苯酚的化学与生物降解法进行了评述.在化学降解法中着重讨论了光催化降解和辐射降解,对比了常用光催化技术(UV,UV/H2O2,UV/H2O2/Fe(Ⅱ/Ⅲ),UV/TiO2)和辐射技术对PCP的降解效率及其影响因素,分析了其降解产物和降解机理.化学降解主要为自由基氧化降解,五氯苯酚在HO·、·O2-等自由基作用下,逐步脱氯生成多酚或醌,然后开环矿化.在微生物降解法中,综述了降解PCP微生物的筛选,论述了PCP在好氧和厌氧条件下的降解过程.五氯苯酚的生物降解路径为:好氧条件下,五氯苯酚在氢氧化酶作用下,被氧化生成氯代醌,并逐步脱去所有的氯原子,生成苯酚后开环;在厌氧和缺氧条件下,五氯苯酚还原脱氯,在得到电子的同时,脱掉一个氯取代基,最终矿化为CH4和CO2.PCP的降解研究对讨论其在环境中的迁移、转化以及含酚废水的处理具有重要意义.     

基于 K-means聚类算法的沥青烟电除尘器火花分析

为了保证沥青烟电除尘器的除尘效率、降低除尘设备的火灾风险,采用了K-means聚类的方法分析ESP放电信号。首先将ESP伏安特性曲线的二维空间进行了分割,确定了不同运行状态与聚类中心的关系,然后使用K-means聚类算法计算其聚类中心,最后根据当前ESP输入参数与各个聚类中心欧氏距离的关系,从而判断出ESP是否处于火花放电状态。仿真结果表明该方法可以准确地判断出所有火花放电信号。     

波茨坦短芽孢杆菌降解间甲酚和4-氯酚的特性

为了高效处理工业含酚废水,研究了波茨坦短芽孢杆菌降解双底物体系过程中间甲酚和4-氯酚的相互作用及苯酚对间甲酚和4-氯酚降解的影响。结果表明,在间甲酚-4-氯酚体系中,4-氯酚会抑制间甲酚的降解,4-氯酚初始质量浓度为40 mg/L时,160 mg/L的间甲酚降解时间延长了8 h;同时间甲酚也抑制4-氯酚的降解,间甲酚初始质量浓度为40 mg/L时,160 mg/L的4-氯酚降解时间延长了4 h。采用Abuhamed动力学方程可以准确描述间甲酚-4-氯酚双底物降解体系中细胞生长的过程,动力学参数I_(1,2)=1.77,I_(2,1)=2.47,决定系数R~2=0.96。拟合参数表明,4-氯酚对间甲酚降解的抑制要强于间甲酚对4-氯酚降解的抑制。酶活测定表明,底物抑制作用增强时苯酚羟化酶和邻苯二酚1,2-双加氧酶的活性降低。添加低质量浓度的苯酚会对间甲酚和4-氯酚的降解产生促进作用,最佳促进质量浓度为200mg/L;添加300 mg/L以上的苯酚会对间甲酚和4-氯酚的降解产生抑制作用,抑制作用随苯酚质量浓度升高而增强。     

丝孢酵母TX1及其固定化降解苯酚特性研究

为研究固定化技术在含酚废水治理中的应用,以聚乙烯醇(PVA)为载体将高效降酚菌株丝孢酵母TX1包埋处理得到胶珠颗粒,在分批培养反应器内分别研究游离体系和固定化体系中溶液p H值、培养温度和苯酚初始质量浓度对TX1降解苯酚效果的影响。结果表明,在游离细胞体系TX1对苯酚降解最佳培养条件为温度30℃,p H=7. 0;而固定化体系中的TX1对苯酚降解的最佳条件为温度30℃,p H=6. 5。在偏酸性条件下,游离细胞体系中TX1对苯酚降解效果比固定化体系差,在25～40℃时后者对苯酚的降解能保持50%以上,表明固定化技术有利于提高微生物的耐受温度。两个体系在降解苯酚过程中均受到底物抑制:在低质量浓度时(≤1 000 mg/L),游离细胞降解速率高于固定化细胞,但当苯酚质量浓度高达3 000 mg/L时,固定化体系中TX1对苯酚比降解速率为0. 088 h-1,远高于前者,表明固定化技术有利于实际高浓度废水的处理。此外,利用高效液相色谱和气相色谱-质谱检测苯酚降解中间产物,只在固定化体系中检测到中间产物为邻苯二酚和顺,顺-黏糠酸。该结果表明,降解过程中固定化体系发生的扩散阻力延迟了体系的降解反应,有利于发现中间体,使固定化技术有望成为新的检测中间体的方法。     

苯酚强降解菌的筛选及温度对降解的影响

以江油市某以石油为原料生产甲醇的甲醇厂污水处理站污泥和分析纯苯酚为原料,通过富集培养,涂布平板法(Spread plate method)和平板划线法(Streak plate method)进行菌株分离,并采用不断加大苯酚质量浓度的方法对PD2菌株置于34 ℃、150 r/min的摇床上进行振荡驯化培养,得到以苯酚为唯一碳源,能降解高酚浓度的优势降酚菌.PD2菌株经过6代驯化后的试验表明: 该菌58 h对质量浓度为1 100 mg/L苯酚的降解率达98.6%,58 h对质量浓度为1 400 mg/L苯酚的降解率达94.3%,60 h对质量浓度为2 200 mg/L苯酚的降解率达83.6%.说明一定范围内提高苯酚的质量浓度可以提高PD2菌株降解苯酚的酶的活性.在不同温度下观察菌株的生长及对苯酚的降解情况,结果表明,该菌最佳降解苯酚温度为34 ℃.     

Experimental study on electrostatic spark discharge under different electrode parameters,pressure and gas component

In this work, the influence of different experimental parameters (electrode gap, electrode shape, pressure and gas component) on spark discharge characteristics is investigated. The dynamic processes of voltage, current, energy, and power during the spark discharge process are analyzed. Electrical characteristic parameters including the discharge energy, discharge efficiency, spark resistance and total resistance are studied. High-speed schlieren technology is used to visualize the spark discharge and shock wave formation under different pressure and electrode shapes. The effect of pressure on the shape, radius and average velocity of the shock wave is investigated.     

混合药物粉尘输运过程静电特性实验研

兽药制药粉尘加工工艺过程中,由于粉尘颗粒之间或颗粒与设备、管壁之间的碰撞、摩擦,导致装置内部静电荷量积聚,激发静电放电,粉尘燃烧或爆炸的事故频发。实验主要通过包括粉尘与管材摩擦的漏电电流测试和静电放电火花对粉尘云点燃敏感性测试两部分。结果表明:单一药物药粉的静电漏电电流随着管材管径的增大,管长的增长,静电漏电电流逐渐变大;随着倾斜角的增大,静电漏电电流先增大后降低;镀锌铁管的漏电电流大于PVC管,电荷逸散速度更快。单一兽药粉的粉尘云放电火花最小点燃能量随质量浓度的变化,呈现二次曲线的变化趋势。混合兽药粉与单一兽药粉的漏电电流和粉尘云放电火花最小点燃能量的测试结果的变化趋势是一致的。     

Testing of dust clouds for the electrostatic-spark ignition hazard in industry. Need for a modified approach?

Current standard test methods for electric-spark minimum ignition energies (MIEs) of dust clouds in air require that a series inductance of at least 1–2 mH be included in the electric-spark discharge circuit. The reason is to prolong the spark discharge duration and thus minimize the spark energy required for ignition. However, when assessing the minimum electrostatic energy ½CU² for dust cloud ignition by accidental electrostatic-spark discharges, current testing standards require that the series inductance of at least 1–2 mH be removed from the spark discharge circuit. No other changes of apparatus and test procedure are required. The present paper questions whether this simple approach is always adequate. The reason is that in practice in industry accidental electrostatic-spark discharge circuits may contain large ohmic resistances due to corrosion, poor electrical grounding connections, poorly electrically conducting construction materials etc. The result is increased spark discharge durations and reduced mechanical disturbance of the dust cloud by the blast wave emitted by the spark. Therefore, testing for minimum ½CU² for ignition by accidental electrostatic spark discharges may not only require removal of the series inductance of 1–2 mH from the standard MIE spark discharge circuit. Additional tests may be needed with one or more quite large series resistances R_s inserted into the spark discharge circuit. The present paper proposes a modified standard test procedure for measurement of the minimum electrostatic-spark ignition energy of dust clouds that accounts for these effects.     

浮顶储罐导电片间隙放电危险性研究

储罐在实际运行中,受浮盘的上下移动、机械应力、老化、油污、金属腐蚀等因素的影响,很难确保导电片与罐壁紧密贴合,容易形成微小间隙,在这种情况下遭受雷击易产生间隙放电,出现打火现象.为了分析导电片与储罐罐壁导电片产生间隙放电的危险性,根据Townsend气体放电理论计算了导电片和储罐罐壁间的击穿电压,采用1.2/50μs冲击电压波开展了导电片间隙放电实验,分析了导电片击穿电压与空气间隙距离的关系.结果证明:当导电片和罐壁贴合不良时,导电片和罐壁之间极易产生火花放电;当空气间隙d=0.1cm时,平均空气击穿电压仅为5280V;随着间隙的增大,空气击穿电压也随之增大;导电片间隙放电实验数据与Townsend气体放电理论值吻合.最后,根据以上结论,针对浮顶储罐导电片间隙放电的危险性,提出了改进措施.     

外浮顶油罐雷击起火概率计

大型外浮顶储罐多次发生雷击起火事故,因此对其安全性做出客观评价,计算雷击起火概率现实意义重大。通过分析雷电对外浮顶油罐的危害方式,利用蒙特卡洛方法结合电气几何模型计算外浮顶油罐年雷击率。分析采用导静电线和可伸缩接地装置（RGA）的防护效果差别。最后计算安装可伸缩接地装置后油罐遭受雷击产生火花放电的年事故率。计算结果表明:年雷击率随着油罐直径和罐壁高度的增大而增加;采用可伸缩接地装置的防护效果明显优于传统导静电线;安装多个可伸缩接地装置可以明显降低产生火花的概率和年事故率。两个RGA就可以将油罐遭受雷击产生火花放电的年事故率降至10-5以下。     

Measurement of minimum ignition energies (MIEs) of dust clouds – History,present, future

Nearly 130 years ago Holtzwart and von Meyer (1891) demonstrated by experiments that explosible dust clouds could be ignited by inductive electric sparks. Then more than half a century passed before the publication of the important quantitative research of Boyle and Llewellyn (1950) and Line et al. (1959). They worked with capacitive electric sparks and found that the minimum capacitor energies ½CU² required for ignition of various dust clouds in air decreased substantially when a large series resistance, in the range 10⁴–10⁷ Ω, was introduced in the discharge circuit. When considering that the net energies of the sparks themselves were only of the order of 10% of the ½CU² discharged, the minimum net spark energies required for ignition with a large series resistance were only a few per cent of the net energies required without such a resistance.Line et al. observed that the essential effect of increasing the series resistance, and hence increasing the discharge time of the sparks, was to reduce the disturbance of the dust cloud by the blast wave from the spark. This phenomenon was explored further by Eckhoff (1970, 2017), and subsequently by some simple experiments by Eckhoff and Enstad (1976). Franke (1974, 1977) and Laar (1980) confirmed the additional finding of Line et al. (1959) that the minimum ½CU² for ignition is also substantially reduced by including a series inductance in the discharge circuit, rather than a series resistance. The basic reason is the same as with a large series resistance, viz. increased spark discharge time and hence decreased disturbance of the dust cloud by blast wave from the spark. For this reason inclusion of an appreciable series inductance in the spark discharge circuit is an essential element in current standard MIE test methods.In experiments with spark ignition of transient dust clouds produced by a blast of air in a closed vessel, it is necessary to synchronize the occurrence of the spark with the formation of the dust cloud. The precision required from this type of synchronization is typically of the order of 10 ms, which can be obtained even by mechanical arrangements, such as rapid change of spark gap length, or of the distance between two capacitor plates. The present paper reviews some methods that have been/are being used for achieving adequate synchronization of dust cloud appearance and spark discharge. Some current standard experimental methods for determining MIEs of dust clouds experimentally have also been reviewed. The same applies to some theories of electric-spark ignition of dust clouds.At the end of paper some suggestions for possible future modifications of current standard methods for measuring MIEs of explosible dust clouds are presented. With regard to justifying significant modifications of existing standard methods, the “bottom line” is, as quite often in many connections, that any modifications should be based on realistic cost/benefit evaluations.     

Characteristics and hazards of electrostatic discharges in air

In the assessment of electrostatic hazards in the process industries, a great deal of emphasis has been placed on the determination of energies in spark discharges. There are, however, other electrostatic discharge phenomena where this approach has severe limitations. The purpose of this paper is to describe the state-of-the-art with respect to electrostatic discharges in gases (air). An in depth review of the literature has been made, and the various types of discharges are tabulated and discussed.     

Experimental investigation of spark ignition energy in kerosene,hexane, and hydrogen

Quantifying the risk of accidental ignition of flammable mixtures is extremely important in industry and aviation safety. The concept of a minimum ignition energy (MIE), obtained using a capacitive spark discharge ignition source, has traditionally formed the basis for determining the hazard posed by fuels. While extensive tabulations of historical MIE data exist, there has been little work done on ignition of realistic industrial and aviation fuels, such as gasoline or kerosene. In the current work, spark ignition tests are performed in a gaseous kerosene–air mixture with a liquid fuel temperature of 60 °C and a fixed spark gap of 3.3 mm. The required ignition energy was examined, and a range of spark energies over which there is a probability of ignition is identified and compared with previous test results in Jet A (aviation kerosene). The kerosene results are also compared with ignition test results obtained in previous work for traditional hydrogen-based surrogate mixtures used in safety testing as well as two hexane–air mixtures. Additionally, the statistical nature of spark ignition is discussed.     

电感性本质安全电路L/R的选择原则

基于电感性本质安全电路放电电流线性衰减模型,引入最小建弧电压的概念,得到了放电时间不含未知参数的表达式,利用电感电路的本质安全性能判别式,确定了电感电阻比L/R的选取原则.     

浮顶储罐二次密封油气空间放电分析

为避免浮顶储罐在遭受雷击时由于导电片设施在二次密封油气空间中放电引起密封圈火灾,在实验室建立了2 m直径油罐模型,开展导电片火花放电起始电流试验、导电片与罐壁形成空气间隙击穿放电初始电压试验,系统研究导电片在二次密封油气空间中的放电危险性。试验结果表明:导电片靠自身弹性与罐壁贴合时,雷电流大约在400 A时导电片开始产生点燃性火花放电;如导电片与罐壁贴合不良形成空气间隙,雷击情况下雷电流泄放瞬时浮顶与罐壁之间的电位差足以使一定大小的间隙击穿放电,当间隙大小为20~30 mm时,放电电压为26~40 kV。因此,储罐在遭受雷击时,导电片火花放电现象不可避免。结合储罐的实际运行情况,提出取消二次密封导电片、液下刮蜡器与浮顶进行可靠电气连接的改进措施,避免导电片在二次密封油气空间中放电发生,大大降低浮顶储罐雷击火灾事故。