Liu Y, Cain J P, Wang H, Laskin A
William R. Wiley Environmental Molecular Sciences Laboratory, Pacific Northwest National Laboratory, PO Box 999, MSIN K8-88, Richland, Washington 99352, USA.
J Phys Chem A. 2007 Oct 11;111(40):10026-43. doi: 10.1021/jp072005p. Epub 2007 Sep 13.
Heterogeneous reaction kinetics of gaseous nitric acid with deliquesced sodium chloride particles NaCl(aq) + HNO3(g) --> NaNO3(aq) + HCl(g) were investigated with a novel particle-on-substrate stagnation flow reactor (PS-SFR) approach under conditions, including particle size, relative humidity, and reaction time, directly relevant to the atmospheric chemistry of sea salt particles. Particles deposited onto an electron microscopy grid substrate were exposed to the reacting gas at atmospheric pressure and room temperature by impingement via a stagnation flow inside the reactor. The reactor design and choice of flow parameters were guided by computational fluid dynamics to ensure uniformity of the diffusion flux to all particles undergoing reaction. The reaction kinetics was followed by observing chloride depletion in the particles by computer-controlled scanning electron microscopy with energy-dispersive X-ray analysis (CCSEM/EDX). The validity of the current approach was examined first by conducting experiments with median dry particle diameter D(p) = 0.82 microm, 80% relative humidity, particle loading densities 4 x 10(4) <or= N(s) <or= 7 x 10(6) cm(-2) and free stream HNO3 concentrations 2, 7, and 22 ppb. Upon deliquescence the droplet diameter D(d) approximately doubles. The apparent, pseudo-first-order rate constant determined in these experiments varied with particle loading and HNO3 concentration in a manner consistent with a diffusion-kinetic analysis reported earlier (Laskin, A.; Wang, H.; Robertson, W. H.; Cowin, J. P.; Ezell, M. J.; Finlayson-Pitts, B. J. J. Phys. Chem. A 2006, 110, 10619). The intrinsic, second-order rate constant was obtained as kII = 5.7 x 10(-15) cm3 molecule(-1) s(-1) in the limit of zero particle loading and by assuming that the substrate is inert to HNO3. Under this loading condition the experimental, net reaction uptake coefficient was found to be gamma(net) = 0.11 with an uncertainty factor of 3. Additional experiments examined the variations of HNO3 uptake on pure NaCl, a sea salt-like mixture of NaCl and MgCl2 (Mg-to-Cl molar ratio of 0.114) and real sea salt particles as a function of relative humidity. Results show behavior of the uptake coefficient to be similar for all three types of salt particles with D(p) approximately 0.9 miccrom over the relative humidity range 20-80%. Gaseous HNO3 uptake coefficient peaks around a relative humidity of 55%, with gamma(net) well over 0.2 for sea salt. Below the efflorescence relative humidity the uptake coefficient declines with decreasing RH for all three sea salt types, and it does so without exhibiting a sudden shutoff of reactivity. The uptake of HNO3 on sea salt particles was more rapid than that on the mixture of NaCl and MgCl2, and uptake on both sea salt and sea salt-like mixture was faster than on pure NaCl. The uptake of HNO3 on deliquesced, pure NaCl particles was also examined over the particle size range of 0.57 <or= D(p) <or= 1.7 microm (1.1 <or= D(d) <or= 3.4 microm) under a constant relative humidity of 80%. The uptake coefficient decreases monotonically with an increase in particle size. Application of a resistance model of reaction kinetics and reactant diffusion over a single particle suggests that, over the range of particle size studied, the uptake is largely controlled by gaseous reactant diffusion from the free stream to the particle surface. In addition, a combined consideration of uptake coefficients obtained in the present study and those previously reported for substantially smaller droplets (D(d) approximately 0.1 microm) (Saul, T. D.; Tolocka, M. P.; Johnston, M. V. J. Phys. Chem. A 2006, 110, 7614) suggests that the peak reactivity occurs at a droplet diameter of approximately 0.7 microm, which is immediately below the size at which sea salt aerosols begin to notably contribute to light scattering.
采用新型的载于基底的滞流流动反应器(PS-SFR)方法,在与海盐颗粒大气化学直接相关的条件下,包括粒径、相对湿度和反应时间,研究了气态硝酸与潮解的氯化钠颗粒之间的多相反应动力学:NaCl(aq) + HNO3(g) --> NaNO3(aq) + HCl(g)。通过反应器内的滞流流动冲击,将沉积在电子显微镜网格基底上的颗粒在大气压和室温下暴露于反应气体中。反应器的设计和流动参数的选择由计算流体动力学指导,以确保扩散通量对所有正在反应的颗粒的均匀性。通过计算机控制的扫描电子显微镜结合能量色散X射线分析(CCSEM/EDX)观察颗粒中氯的消耗,从而跟踪反应动力学。首先通过对中位干颗粒直径D(p) = 0.82微米、相对湿度80%、颗粒负载密度4×10⁴≤N(s)≤7×10⁶ cm⁻²以及自由流HNO3浓度为2、7和22 ppb进行实验,检验了当前方法的有效性。潮解后液滴直径D(d)大约翻倍。在这些实验中确定的表观拟一级速率常数随颗粒负载和HNO3浓度而变化,其方式与早期报道的扩散动力学分析一致(拉斯金,A.;王,H.;罗伯逊,W. H.;考因,J. P.;埃泽尔,M. J.;芬利森-皮茨,B. J.《物理化学杂志A》2006年,110卷,10619页)。在零颗粒负载的极限情况下,并假设基底对HNO3呈惰性,得到本征二级速率常数为kII = 5.7×10⁻¹⁵ cm³ 分子⁻¹ s⁻¹。在此负载条件下,实验测得的净反应吸收系数为γ(net) = 0.11,不确定因子为3。另外的实验研究了HNO3在纯NaCl、NaCl和MgCl2的类海盐混合物(Mg与Cl的摩尔比为0.114)以及真实海盐颗粒上的吸收随相对湿度的变化。结果表明,在20 - 80%的相对湿度范围内,对于所有三种粒径约为0.9微米的盐颗粒,吸收系数的行为相似。气态HNO3吸收系数在相对湿度约为55%时达到峰值,对于海盐,γ(net)远超过0.2。在低于风化相对湿度时,对于所有三种海盐类型,吸收系数随相对湿度降低而下降,并且下降过程中没有表现出反应性的突然终止。HNO3在海盐颗粒上的吸收比在NaCl和MgCl2混合物上更快,并且在海盐和类海盐混合物上的吸收都比在纯NaCl上更快。在80%的恒定相对湿度下,还研究了HNO3在粒径范围为0.57≤D(p)≤1.7微米(1.1≤D(d)≤3.4微米)的潮解纯NaCl颗粒上的吸收。吸收系数随粒径增加而单调下降。对单个颗粒上反应动力学和反应物扩散的阻力模型的应用表明,在所研究的粒径范围内,吸收主要由气态反应物从自由流到颗粒表面的扩散控制。此外,综合考虑本研究中获得的吸收系数以及先前报道的对于小得多的液滴(D(d)约为0.1微米)的吸收系数(索尔,T. D.;托洛卡,M. P.;约翰斯顿,M. V.《物理化学杂志A》2006年,110卷,7614页)表明,峰值反应性出现在液滴直径约为0.7微米处,这刚好低于海盐气溶胶开始对光散射有显著贡献的尺寸。