离心系数表征丙烯酰胺反相乳液的稳定性

用丙烯酰胺反相乳液经离心处理后保留的乳液体积与原乳液体积之比（离心系数Vr）考察了丙烯酰胺及其衍生物反相乳液的稳定性。 结果表明,离心系数Vr越大,其乳液的稳定性越好。 在高速离心条件下,由Span80/Span85和Tween80构成的丙烯酰胺及其衍生物反相乳液的Vr与油相质量分数存在正相关的关系。 在油相质量分数确定的情况下,离心系数Vr不仅与3种表面活性剂构成的亲水亲油平衡值（HLB）有关,而且与丙烯酰胺及其衍生物的浓度和类型有关。 HLB值在4.20左右时,乳液是稳定的;随丙烯酸氧乙基三甲基氯化铵（DAC）在水相中质量分数的提高,反相乳液稳定性增强,w(DAC)＞24%时可得到稳定乳液。 在15000 r/min离心3 min,Vr=0.95以上的丙烯酰胺及其衍生物反相乳液很稳定,静置半年仍未出现分层现象。     

影响反相微乳液导电性能的因素

分别以聚乙二醇辛基苯基醚(Triton X-100)或十六烷基三甲基溴化铵(CTAB)为表面活性剂, 与正己烷、正己醇和水构成反相微乳液. 研究了水相H+浓度、表面活性剂、助表面活性剂等对微乳液导电性能的影响. 结果表明, 增加水相H+浓度可大幅度提高反相微乳液的导电能力, 当H+浓度由1.0 mol•L-1增加到10 mol•L-1时, 微乳液的电导率可提高1~2个数量级. 当水相H+浓度为10 mol•L-1时, 微乳液的电导率随溶水量的增大而增大, 水油体积比为3:10时, 两种体系的电导率均达到3200 μS•cm-1. Triton X-100浓度对微乳液的电导率影响较大, 电导率随其浓度增加而增大；而CTAB浓度对微乳液电导率的影响较小, 电导率随其浓度增加略有减小；助表面活性剂正己醇使非离子型反相微乳液的电导率下降, 而使阳离子型反相微乳液的电导率先增大, 然后减小, 呈骆峰状变化.     

Pickering乳液法制备聚苯胺-石墨烯空心微球

通过对石墨烯进行磺酸化改性使其具有双亲性,以改性后的磺化石墨烯（SGR）作为Pickering乳化剂稳定含有苯胺的油相,加入过硫酸铵引发剂,采用Pickering乳液聚合的方式一步合成具有独特空心结构的聚苯胺-石墨烯微球（PANI-SGR HS）.详细探究了石墨烯磺化程度、乳化剂浓度和油水比等因素对磺化石墨烯稳定乳液的影响,研究结果表明：SGR的润湿性对Pickering乳液的稳定性有着重要影响;SGR浓度为0.5 mg·mL^-1时即可以稳定乳液,随着SGR浓度的增大,Pickering乳液滴尺寸呈减小趋势;在油相体积分数小于60%时,即可以得到比较稳定的乳液.利用扫描电子显微镜对微球的形貌进行了表征,并对所制备空心微球的电化学性能进行了探究,在电流密度为1 A·g^-1时,其修饰电极的比电容可达480.59 F·g^-1,相比于普通二维PANI-SGR提高了103.5%.     

油酸-正丙醇-水无表面活性剂反相微乳液电导研究

本文对油酸-正丙醇-水三元体系的相行为进行了研究,表明可形成微乳液.由于体系中无传统表面活性剂,故所形成的微乳液为无表面活性剂微乳液.在反相微乳液区,固定正丙醇/油酸体积比(RP/O)为3∶5、1∶1和2∶1,考察了体系电导率(κ)随分散相体积分数(φd)的变化,结果表明κ随φd的增大先缓慢增加,后急剧增大,符合渗滤特...     

羧甲基丝素的制备工艺优化及其乳化性能

以废丝为主要原料,将不溶于水的丝素蛋白通过与一氯乙酸在乙醇溶剂中的醚化反应,合成了可溶性的羧甲基丝素。讨论了几种主要因素(如碱化时间、碱化温度、醚化时间和醚化温度等)对产物醚化度的影响,得到了制备羧甲基丝素的醚化工艺条件:碱化时间90 min、醚化时间90 min、碱化温度25℃、醚化温度70℃。所得羧甲基丝素的醚化度为0.7425。测定羧甲基丝素的表面活性后,得到羧甲基丝素的临界胶束浓度为1.25 g/L,亲水亲油平衡(HLB)值为10。丝素蛋白溶液具有一定的起泡能力,且在质量分数为1.0%～1.2%范围内的稳定性较好,但不宜作发泡剂。丝素蛋白溶液具有良好的乳化能力和乳化稳定性,可作为良好的乳化剂。     

核交联型双亲聚合物胶体粒子的制备及其乳化性能

以三硫代碳酸酯为链转移剂,合成了端羧基聚(丙烯酸-r-苯乙烯)(P(AA-r-St))大分子链转移剂;将其用于二乙烯基苯的可逆加成-断裂链转移自由基(RAFT)聚合,一步制备了以交联聚二乙烯基苯为内核、P(AA-r-St)为核外大分子链的双亲聚合物胶体粒子。通过红外光谱、核磁共振氢谱和凝胶渗透色谱确定了大分子链转移剂的化学结构;采用纳米粒度仪、扫描电子显微镜和水接触角测试对胶体粒子的尺寸、形貌及亲-疏水性进行了表征。研究了核外大分子链的化学组成、水相pH、油-水体积比以及油相类型对胶体粒子乳化性能的影响,并通过油相固化的方式考察了胶体粒子在油-水界面的形貌。结果表明:改变核外大分子链的化学组成可有效调控胶体粒子的尺寸、亲-疏水性及乳化性能;当核外大分子链中疏水基元St的物质的量分数为11%时,胶体粒子能够在较宽的pH范围(3~11)稳定水包油型乳液,最大油相体积分数达66.7%;胶体粒子吸附于油-水界面上,有效阻止了乳液滴的聚并;此外,胶体粒子可长效稳定多种油-水体系,作为颗粒乳化剂具有良好的普适性。     

淀粉乳液形成过程主要影响因素的耗散粒子动力学模拟与实验

以环己烷为油相、淀粉乳液为水相、Span60和Tween60为乳化剂, 用耗散粒子动力学(DPD)方法研究了淀粉乳液形成过程及油水比、乳化剂用量等因素对淀粉乳液形成的影响. 结果表明, 模拟6000步时, 体系达到平衡状态; 乳滴的粒径随乳化剂含量的增加先减小而后增加, 随淀粉含量的增加而增加, 随环己烷含量的减小而增加; 形成稳定淀粉乳液体系的参数范围: 7＜油水比≤20, 9%＜乳化剂用量≤18%. 实验结果表明, 乳化剂含量为11%～15%时, 微球的粒径随乳化剂含量的增大而减小; 乳化剂含量大于15%时, 微球的粒径反而增大. 实验与模拟的结果吻合.     

马来松香酸和纳米氧化铝颗粒协同稳定具有pH响应性的Pickering乳液

使用有机颗粒稳定Pickering乳液受到越来越多的关注, 润湿性可调的有机颗粒且结合纳米无机颗粒协同稳定不同类型的Pickering乳液却鲜有报道. 系统研究了基于具有多羧酸基团的松香基衍生物马来松香(MPA)与纳米Al₂O₃颗粒在不同pH条件下形成的乳液类型及相关机理. 研究发现, 在单一MPA颗粒体系条件下, pH可以诱导乳液的类型由W/O Pickering乳液到O/W Pickering乳液, 到最后O/W乳液的转变, MPA的亲水性随着pH升高而增强是该乳液转变的原因. 当纳米Al₂O₃颗粒加入到MPA中后, 吸附在MPA颗粒上的亲水性Al₂O₃导致MPA颗粒亲水性增加, 从而可以使W/O Pickering乳液转变为O/W Pickering乳液(pH=1). 当pH=6时, MPA分子与纳米Al₂O₃颗粒同时具有较强的亲水性且分别无法形成稳定的乳液, 但两者的混合体系可以形成稳定的W/O Pickering乳液, 这是因为MPA分子与纳米Al₂O₃颗粒可以在水溶液中形成疏水性较强的络合物. 另外, 研究了MPA浓度及油相体积分数对乳液外观及粒径的影响, 发现随着MPA浓度增加Pickering乳液的粒径逐渐减小, 增加油相的体积分数会引起粒径的增大. 最后, 利用Zeta电势、颗粒在油水界面吸附率、接触角及表/界面张力研究了稳定Pickering乳液的稳定机理, 在油水界面上吸附的类似盔甲状颗粒层及颗粒层之间形成的网状结构是乳液液滴保持稳定的原因. 为Pickering乳液的绿色化制备提供了一种新的途径, 将在化妆品、医药及新材料等领域得到重要应用.     

1, 1, 2, 3-四氯丙烷乳液消除反应的动力学研究

研究了1,1,2,3-四氯丙烷的乳液消除反应动力学.此反应是二级反应,主要产物是1,1,3-三氯丙烯-2,并有少量顺式及反式-1,2,3-三氯丙烯.从实验发现一系列独特的界面反应特征:(a)乳液消除反应速度常数-表面活性剂浓度图的实验点符合折线关系,折线交点落在某一临界表面活性剂浓度上;(b)表观活化能随表面活性剂浓度的增高而先呈线性增大,达极大值后又急剧下降,最后趋近极限值;(c)表观速度常数K_td几乎不随分散相对分散介质体积的分数变化而改变;(d)反应速度常数的对数随水相离子浓度对数的增大而下降.     

离子液体微乳液合成纳米AgCl及AgCl/poly(MMA-co-St)杂化膜性能调控

在以离子液体氯化-1-十二烷基甲基咪唑(C12mimCl)为表面活性剂,甲基丙烯酸甲酯(MMA)与苯乙烯(St)混合物为油相介质的反相微乳液中合成AgCl纳米粒子,进而采用微乳液原位聚合法制备AgCl/poly(MMA-co-St)杂化膜。通过紫外可见光谱和透射电镜分析了微乳液组成(油相介质组成和增容水量ω)对纳米AgCl粒子形貌的影响。结合扫描电镜和苯、环已烷的溶胀实验探讨了微乳液组成对杂化膜性能的调控作用。结果发现,微乳液油相介质中St/MMA体积比增大有利于在微乳液和杂化膜中获得更多纳米AgCl粒子,增加了杂化膜的苯平衡溶胀吸附量(A∞,b)与苯/环已烷的平衡溶胀吸附选择性(αs,b/c)。在St/MMA体积比为1∶3时杂化膜的A∞,b和αs,b/c分别达到330 mg·g-1和19.21;但过多苯乙烯加入油相介质,其苯环中π键会破坏水核中AgCl粒子的稳定性而引起粒子团聚,从而降低了杂化膜的A∞,b和αs,b/c。反相微乳液中合成的纳米AgCl粒子量随ω增大而增多、粒径增大,杂化膜的A∞,b和αs,b/c随ω的增加而增大。但过高的ω导致微乳液中出现AgCl大粒子,从而引起杂化膜的A∞,b和αs,b/c下降。     

Interfacial rheology of natural silk fibroin at air/water and oil/water interfaces

The interfacial viscoelastic behavior of natural silk fibroin at both the air/water and oil/water interfaces is reported. This natural multiblock copolymer is found to be strongly amphiphilic and forms stable films at these interfaces. The result is an interfacial layer that is rheologically complex with strong surface elastic moduli that are only slightly frequency-dependent. The kinetics of surface viscoelastic evolution are reported as functions of time for various concentrations of the spread films. Films deposited by Langmuir-Blodgett deposition were studied by scanning electron microscopy (SEM) to reveal a fibrous structure at the interface. The production of stable O/W emulsions by silk fibroin further confirms the generation of the elastic films at the oil/water interfaces.     

Emulsification using micro porous glass (MPG): surface behaviour of milk proteins

To investigate the emulsifying properties and adsorption behaviour of high molecular amphiphilic substances such as proteins, it is important to maintain the native status of the used samples. The new method of micro porous glass (MPG) emulsification could offer an opportunity to do this because of the low shear forces. The oil-in-water emulsions were produced by dispersing the hydrophobic phase (liquid butter fat or sunflower oil) through the MPG of different average pore diameters (d_p=0.2 or 0.5 μm) into the flowing continuous phase containing the milk proteins (from reconstituted skim milk and buttermilk). The emulsions were characterised by particle size distribution, creaming behaviour and protein adsorption at the hydrophobic phase. The particle size distribution of protein-stabilised MPG emulsions is determined by the pore size of MPG, the velocity of continuous phase (or wall shear stress σ_w) and the transmembrane pressure. A high velocity of =2 m s⁻¹ (σ_w=13.4 Pa) and low pressure (pressure of disperse phase slightly exceeded the critical pressure Δp_TM=4.5 bar of 0.2 μm-MPG) led to the smallest droplet diameter. As a consequence of average droplet diameters of d₄₃>3.5 μm creaming was observed without centrifugation in all MPG emulsions after 24 h, but no coalescence of the oil droplets occurred. The study of protein adsorption showed that the MPG emulsification at low shear forces resulted in lower protein load values (2.5±0.5 mg m⁻²) than pressure emulsification (11.5±1.0 mg m⁻²). In addition, the various emulsification conditions (MPG or pressure homogenization) led to differences in the relative proportions of casein fractions, whey proteins and milk fat globule membranes (MFGM) at the fat globule surfaces.     

Release properties on gelatin-gum arabic microcapsules containing camphor oil with added polystyrene

In this study, gelatin blended with arabic gum microcapsules containing camphor oil with added polystyrene were fabricated by a compound coacervation method. The parameters of oil/wall volume ratio, emulsification stirring speed, concentration of cross-linking agent, treated time and oil release properties were investigated. In order to improve the constant release effect of camphor oil, oil-soluble polystyrene (PS) was used as a sustained release agent. The camphor oil release curves were expressed by the exponential equation: ψ(t) = C_eq(1–e^−t/τ), where ψ(t) represent the variant of camphor oil concentration in the operation environment, C_eq as the equilibrium state, t as the release time and τ as time constant. C_eq and τ are significant factors pertaining to the camphor oil release properties. The results indicated that, for the microcapsules, the optimal oil/wall volume ratio was 0.75 to achieve the encapsulation efficiency of 99.6 wt.%. The average particle size were 294.7 ± 14.2 μm, 167.2 ± 11.2 μm, 85.7 ± 8.7 μm at the homogenization stirring speed of 500, 1000, and 2000 rpm, respectively. The effect of sustained oil release will increase whereas the stirring speed decreases and the concentration of glutaraldehyde (GA) and treated time increases. Along with the increasing of quantity of polystyrene added, C_eq decreased and τ increased, indicating that the sustained oil release amount and the release rate depend on the quantity of PS considerably.     

Spreading of oil from protein stabilised emulsions at air/water interfaces

Spreading of a drop of an emulsion made with milk proteins on air/water interfaces was studied. From an unheated emulsion, all oil molecules could spread onto the air/water interface, indicating that the protein layers around the oil globules in the emulsion droplet were not coherent enough to withstand the forces involved in spreading. Heat treatment (90 °C) of emulsions made with whey protein concentrate (WPC) or skim milk powder reduced the spreadability, probably because polymerisation of whey protein at the oil/water interface increased the coherence of the protein layer. Heat treatment of emulsions made with WPC and monoglycerides did not reduce spreadability, presumably because the presence of the monoglycerides at the oil/water interface prevented a substantial increase of coherence of the protein layer. Heat treatment of caseinate-stabilised emulsions had no effect on the spreadability. If proteins were already present at the air/water interface, oil did not spread if the surface tension (γ) was <60 mN/m. We introduced a new method to measure the rate at which oil molecules spread from the oil globules in the emulsion droplet by monitoring changes in γ at various positions in a ‘trough’. The spreading rates observed for the various systems agree very well with the values predicted by the theory. Spreading from oil globules in a drop of emulsion was faster than spreading from a single oil drop, possibly due to the greater surface tension gradient between the oil globule and the air/water interface or to the increased oil surface area. Heat treatment of an emulsion made with WPC did not affect the spreading rate. The method was not suitable for measuring the spreading rate at interfaces where surface active material is already present, because changes in γ then were caused by compression of the interfacial layer rather than by the spreading oil.     

双核茂金属催化剂的合成、表征与应用

使用桥连配体锂盐与MCl₄络合, 合成了4个不同结构的双核茂金属化合物[μ,μ-(CH₂)₃]{[C(H)·(η⁵-C₅H₄)(η⁵-C₁₃H₈)](MCl₂)}₂[M=Zr or Ti](4, 5)和[μ,μ-(CH₂)₃]{[C(H)(η⁵-C₅H₄)(η⁵-C₉H₆)]·(MCl₂)}₂[M=Zr or Ti](6, 7), 配体和化合物都经过核磁氢谱(¹H NMR)、 碳谱(¹³C NMR)、 红外光谱(IR)及元素分析等表征, 确认了化学结构. 以甲基铝氧烷(MAO)为助催化剂, 化合物4~7为催化剂催化丙烯聚合, 考察了聚合温度、 乙烯压力、 铝钛或铝锆比对催化剂活性及聚合物分子量的影响. 结果表明, 多亚甲基桥连双核茂金属是高活性乙烯和丙烯聚合催化剂, 乙烯聚合活性最高达到7.5× 10⁶ g PE/(mol Zr·h)(化合物6), 丙烯聚合活性达 10 × 10⁵ g sPP/(mol Zr·h)(化合物4). 所得间规聚丙烯(sPP)的间规度指数(SI, r) 达到90%. 在同样条件下, 双核化合物的催化活性、 聚合物分子量M_w(> 100000)以及分子量分布(MWD>2.5)均比相应的单核化合物高(M_w<70000, MWD≤2), 表明该体系中存在较强的核效应.     

宏观均相多孔电极电化学阻抗谱基础

电化学阻抗谱可用于诊断多孔电极内电荷转移反应,即界面电荷集聚和电荷传导,以及反应物质输运。本文采用复相量方法,在同态假设条件下,重新推演多孔电极阻抗谱模型,厘清传统多孔电极阻抗谱模型中的模糊性表述。(1) 定义多孔电极表征输入参数,包括电极基体电子电导率σ₁ 、电解质离子电导率σ₂、界面电荷传递电导率g_ct、单位面积界面电容C、固相扩散系数D、速度常数k、电极厚度d、特征孔深L_p 和单位体积表面积S_c;(2) 解析阻抗谱特征输出参数,包括场扩散常数K,特征频率ω₀、ω₁、ω₂、ω₃和 ω_max,它们分别相关于界面传导反应、有限场扩散、氧化还原反应、孔内扩散和最小特征孔尺寸,以及分别对应于从传导到扩散和从扩散到饱和的转折频率f_k1 和f_k2;(3) 当参数X和Z同时变化时(X = σ₁和Z = d,S_c,L_p,C,g_ct,D,k),通过阻抗谱特征参数的演变规律,分析了电荷转移反应中X和Ζ参数耦合竞争;(4)为深入分析电荷转移反应中参数X和Z的耦合竞争,引入了分叉频率f_XZ和f_ZX 。f_XZ和f_ZX所处位置可以用于表征参数X和Z影响电荷转移反应的深度和广度。当分叉频率f_XZ和f_ZX不存在时,表明电荷转移反应中参数X和Z在全频率范围内存在耦合竞争。总之,借助于特征频率和分叉频率,本文一方面研究了动力学参数和微观结构参数对多孔电极中电荷转移反应的影响,另一方面分析谱图的变化及其背后的阻抗谱特征演化规律。本文研究结果可为阻抗谱的系统仿真和辨识提供理论基础,可为多孔电极内电荷转移反应的竞争分析提供技术支撑,还可为电化学储能系统的优化设计提供诊断工具。     

γ-AlOOH纳米棒的水热合成与形貌调控

γ-AlOOH作为液相法合成γ-Al₂O₃的前驱体,其形貌与最终产物的性能密切相关。 本文采用水热法合成γ-AlOOH纳米棒,通过改变Al³⁺浓度和沉淀剂的种类调控γ-AlOOH纳米棒的长径比,利用X射线衍射仪(XRD)和透射电子显微镜(TEM)表征产物的晶体结构和形貌。 结果表明,随Al³⁺浓度增大可得到长径比在5.9~8.0的γ-AlOOH纳米棒,而改变沉淀剂的种类可进一步将长径比增大到8.0~10.0。 通过对产物结晶过程的分析,发现增大Al³⁺浓度和增强沉淀剂碱性均可以促进铝离子与羟基的配合。 提高反应体系中Al(OH)₃浓度,有利于γ-AlOOH晶粒的成核,促进了晶核之间的定向接触,从而提高了纳米棒的长径比。 长径比为10.0的γ-AlOOH纳米棒烧结所得纳米γ-Al₂O₃改性变压器油(体积分数为0.1%)的正冲击击穿强度较纯油提高9.9%.     

Spreading of partially crystallized oil droplets on an air/water interface

The influence of crystalline fat on the amount and rate of oil spreading out of emulsion droplets onto either a clean or a protein-covered air/water interface was measured for β-lactoglobulin stabilized emulsions prepared with either anhydrous milk fat or a blend of hydrogenated palm fat and sunflower oil. At a clean interface, liquid oil present in the emulsion droplets was observed to completely spread out of the droplets unimpeded by the presence of a fat crystal network. Further, the presence of a fat crystal network in the emulsion droplets had no effect on the rate of oil spreading out of the droplets. At a protein-covered interface, the spreading behavior of emulsion droplets containing crystalline fat was evaluated in terms of the value of the surface pressure (Π_AW) at the point of spreading; Π_AW at spreading was unaffected by the presence of crystalline fat. We conclude it is unlikely that the role of crystalline fat in stabilizing aerated emulsions such as whipped cream is to reduce oil spreading at the air/water interface. However, the temperature of the system did have an effect: spontaneous spreading of emulsion droplets at clean air/water interfaces occurred for systems measured at 5 °C, but not for those measured at 22 or 37 °C. Thus, temperature may play a more important role in the whipping process than commonly thought: the entering and spreading of emulsion droplets was favored at lower temperatures because the surface pressure exerted by protein adsorbed at the air/water interface was reduced. This effect may facilitate the whipping process.     

α,β,γ,δ,ε,η-Bi2O3电子结构和光学性质的第一性原理研究

基于密度泛函理论的CASTEP模块研究了α, β, γ, δ, ε和η-Bi₂O₃晶型, 计算分析了其几何结构、 能带结构、 电子态密度和光学性质. 结果表明, α, ε和η相均为层状结构, 其中, α和ε相为单层—Bi—O—结构, 而η相为双层—Bi—O—结构; β, γ和δ相为—Bi_m—O_n—交错结构, 其中δ相交错尤为密集, 呈现导体特性. 各晶相的导带均由Bi 6p态构成, 价带由O_2p态起主导作用. 电势电位分析结果表明, 6种晶相价带电位均在H₂O/O₂之下, 具有强氧化能力, 与实验报道的光催化氧化能力大小顺序γ-Bi₂O₃>β-Bi₂O₃>α-Bi₂O₃>δ-Bi₂O₃一致, 而导带还原电位低于H₂/H₂O, 预测纯Bi₂O₃很难具备催化产氢能力. 光学性质分析发现, γ和δ相的起始响应波长较大, 说明其应具备红外激发的性质. 这些结果可为获得偏红外激发和较宽光谱响应的Bi₂O₃材料研究提供理论基础, 为研发和应用Bi₂O₃及其复合物提供重要的指导.     

改性钛基PbO2电极的制备及其对COD的快速检测

通过制备Ti/α/β-PbO₂、Ti/Ag/β-PbO₂这两种含有不同中间层的钛基二氧化铅电极来探究电催化氧化技术快速测定葡萄糖模拟废水中有机物(COD)含量的可行性。为了评估两种电极的各项性能,首先采用扫描电镜(SEM)、X射线衍射(XRD)对电极进行形貌表征,其次进行电化学性能测试包括线性伏安曲线(LSV)、塔菲尔曲线(Tafel)、循环伏安曲线(CV)以及交流阻抗测量分析。结果表明,Ti/α/β-PbO₂电极表面晶体结构更加均匀,晶粒尺寸偏小,具有更大的电活性表面积。Ti/α/β-PbO₂电极的析氧电位为1.77 V,为·OH的产生提供良好条件。在Tafel、CV测试中,Ti/α/β-PbO₂电极的交换电流密度i₀及比电容C_p分别为0.0995 A·cm^-1、0.004098 F·cm^-1均高于Ti/Ag/β-PbO₂电极,说明Ti/α/β-PbO₂电极的耐腐蚀性以及释放电子的能力优异。最终选用Ti/α/β-PbO₂电极为工作电极。Ti/α/β-PbO₂电极检测COD的最佳条件为：氧化电位1.30 V、电解时间150 s、电解液浓度0.03 mol·L^-1 硝酸钠(NaNO₃)。电化学法与比色消解法测定COD的相关系数可达0.9909,同时具有良好的重现性与相关性,COD的检测范围为0 mg·L^-1 ~ 500 mg·L^-1。在误差允许的范围内可以替代标准的重铬酸钾法,为实现COD的在线快速检测提供参考价值。