原位漫反射FTIR研究Fe改性的Cu-Mn/ZrO_2催化剂上CO的吸附行为

利用原位漫反射傅里叶变换红外光谱(FTIR)技术,研究了Fe改性的Cu-Mn/ZrO_2催化剂的CO吸附行为。通过测定单组元及其不同组合催化剂的CO吸附以及催化剂的CO-TPD-IR特征、不同温度CO吸附的红外光谱,研究了Fe助剂对催化剂上CO吸附行为的影响,发现Fe通过提高铜的分散度,改变铜的化学环境,影响催化剂上CO线式吸附的特征,而且形成CO桥式吸附中心,从而提供了低碳醇合成的催化剂表面,并探讨了催化剂上CO吸附形式变化的规律。     

掺杂碱金属与碱土金属的CuO-CeO_2催化剂的漫反射红外光谱分析

CuO-CeO2系列催化剂是高效的CO选择性氧化反应的催化剂,通过原位漫反射红外光谱对掺杂碱金属和碱土金属氧化物的CuO-CeO2催化剂表面的吸附物种进行了研究。结果表明CuO-CeO2系列催化剂上,2 106 cm-1处出现CO的红外吸附峰。在反应气氛中,此峰的强度随着温度先升高后降低,说明Cu+是CO主要的活性吸附中心。低温下催化剂表面吸附的CO主要以可逆形式脱附出来,而高温下CO则以不可逆的形式脱附出来。催化剂表面在3 660 cm-1处出现尖锐的红外峰,归属于CeO2经还原产生的Ce-(OH)2偕式基团。在1 568,2 838和2 948 cm-1附近处出现甲酸根的红外谱峰,以及1 257和1 633 cm-1处出现碳酸根物种的红外峰。甲酸根物种是气相的CO与表面的羟基反应生成的产物,该物种的C—H键断裂生成碳酸根物种,这两物种均会降低催化剂的高温活性。Cu1Li1Ce9Oδ催化剂出现较强的CO2和甲酸根的红外峰,温度高于180℃时,该催化剂上还能看到微弱的CO红外峰,说明锂离子的给电子性质有利于提高Cu1Li1Ce9Oδ催化剂上CO的不可逆脱附,抑制氢的活化吸附,同时促进了甲酸根物种的生成。低温下Cu1Mg1Ce9Oδ和Cu1Ba1Ce9Oδ催化剂上CO的吸附量较多,但主要以可逆脱附形式脱附出来,对CO选择性氧化没有贡献。     

不同添加物对CO在Ru/Al_2O_3上吸附态的影响

利用红外光谱技术考察了吸电性添加物(Cl~-,Br~-和I~-)及给电性添加物(Na_2O和K_2O)对CO在Ru/Al_2O_3催化剂上吸附态的影响。发现添加物不同时,CO吸收谱带的数目、位置及强度均有变化。同时考察了添加物浓度和吸附温度的影响,观察到添加物Cl~-与残留Cl~-对CO吸附的不同作用。     

甲醇在γ-Al2O3,CeO2及其负载Pd催化剂上吸附和分解的原位红外光谱研究

利用原位傅里叶变换红外光谱 (FTIR)技术对甲醇在γ Al2 O3,CeO2 以及Pd/Al2 O3,Pd/CeO2 催化剂上的吸附和分解行为进行了研究。综合考虑了载体和活性组分的作用 ,分析了甲醇在不同载体负载Pd催化剂上可能的分解途径。在Pd/CeO2 催化剂上 ,活性组分和载体对甲醇分解的过程表现出了一种协同效应。     

臭氧在SnO2表面吸附的红外光谱研究

以SnO2催化臭氧化降解高浓度糖蜜酒精废水为探针反应,研究SnO2催化臭氧化降解糖蜜酒精废水的活性,并采用红外光谱研究臭氧在SnO2及金属氧化物改性的SnO2催化剂表面的吸附行为。结果表明:由纯氧源制得的O3在SnO2表面吸附的红外光谱上的1 027和1 055 cm-1及2 099和2 122 cm-1处存在两处明显的吸收双峰,而空气制备的O3在SnO2表面与CO及CO2等存在竞争吸附,使得O3的吸附减少,催化臭氧化降解糖蜜废水的降解率下降。催化剂助剂对SnO2催化臭氧化降解糖蜜酒精废水有较大的影响。采用Fe2O3,NiO,CuO,ZnO,MgO,SrO及BaO等金属氧化物为助剂改性的SnO2在2 236和2 213 cm-1,1628和1 599 cm-1出现强度相似的吸收峰,但是几种催化剂对CO2和CO的吸附差别较大,过渡金属改性的SnO2在1 580~1 070 cm-1处出现较宽的吸收峰,碱土金属氧化物改性的SnO2催化剂在1 580~1 070 cm-1之间,出现了1 298和1 274 cm-1两个新的峰,从而引起了不同助剂催化臭氧化的活性差别,碱土金属改性的SnO2对糖蜜酒精废水的催化臭氧化脱色效果明显优于过渡金属改性的SnO2,其中BaO改性的SnO2催化剂的活性最好。     

CO探针原位红外光谱研究Pt/Sn双金属重整催化剂

催化重整是生产芳烃原料和高辛烷值清洁汽油调和组分的重要工艺。以目前应用广泛的铂锡工业重整催化剂金属含量为参比,用工业剂制备方法合成了Pt含量为0.6%的一系列铂锡重整催化剂,建立CO探针原位红外的表征方法,并对其进行系统表征,首次获得了1%以下低含量助剂Sn的CO探针红外谱图。研究结果表明,系列剂的金属Pt的CO吸附特征峰主要以线式吸附状态存在。0.6%纯Pt剂上1 826 cm-1处CO桥式吸附特征峰,因添加助剂Sn后,强度下降,而CO线式吸附特征峰的强度则增加,说明Sn的加入使得Pt的分散度增加。变温CO探针吸附原位红外研究表明,对负载质量分数0.3%的纯Sn催化剂,当脱附温度升高至120 ℃时,吸附在Sn上的CO特征峰会完全消失。对负载质量分数0.6%的纯Pt催化剂,当脱附温度升高至300℃时,吸附在Pt中心上的CO特征峰会完全消失。当Pt-Sn双金属负载质量分数Pt为0.6%、Sn为0.3%时,CO的脱附温度明显提高达350 ℃。与纯Pt剂相比,随着Sn助剂的加入,使得CO的脱附温度稍有提升,Pt-Sn催化剂Pt的CO特征峰向高波数方向移动,说明Sn的加入一定程度上减弱了活性金属Pt中心上的电荷密度。因而,CO探针原位红外是表征低金属铂锡工业重整催化剂的有效手段,为阐明多金属重整催化剂的助剂作用和研究反应机理提供重要信息。     

原位红外光谱法研究大气颗粒物表面非均相反应

大气污染物之间可能发生协同作用,造成严重的二次污染,产生次生环境问题.本实验通过原位红外光谱分析方法研究气态污染物和碳颗粒物之间的吸附过程,发现大气中CO2和NO极易在颗粒物表面发生吸附;CO2在颗粒物表面达到吸附平衡时间很短,NO的吸附平衡时间较长;CO2和SO2会影响NO在颗粒物表面的吸附,CO2在颗粒物表面的吸附几乎不受NO和SO2的影响.     

Pd修饰Cu电极的电化学CO_2还原（英文）

利用微分电化学质谱和电化学原位衰减全反射红外光谱技术探究了Cu和CuPd催化剂上CO_2和CO的电化学还原行为.红外光谱观察到了生成甲醇、甲烷与乙烯的CH_x中间物种.在CuPd电极CO_2还原过程中,红外光谱的CO吸附峰起始电位比Cu正移大约300 mV,说明CuPd能够有效促进CO_2还原;CO饱和溶液中,Cu和CuPd电极CO起始吸附电位基本相同;两电极上CO谱带出现的电位与CO_3~(2-)的谱带降低的电位基本相同,说明C O的吸附需要CO_3~(2-)的脱附.利用电化学在线质谱发现在CuPd电极上CO还原产生CH_4和CH_3OH的起始电位比Cu电极正移约200 mV.推测催化活性的提升可能是由于Pd的引入改变了Cu的d能带,且Pd吸附更多的H,从而促进CO_2还原,使CO能够与H结合并被深度还原.     

不同温度下乙醇电氧化过程的原位红外光谱研究

直接乙醇燃料电池因其优异的性能备受关注。乙醇的电催化氧化并非简单的燃烧,涉及多种催化反应过程。乙醇的C-C键断裂选择性低,以及乙醇氧化中间产物C1分子由于没有及时氧化离开催化剂表面而造成的催化剂中毒,是制约其应用的瓶颈问题。电化学原位红外光谱是在电化学反应的同时,原位采集反应物种特定官能团的振动信息,可在分子水平揭示反应过程,推测反应机理。不同温度条件下乙醇电氧化过程的研究,有助于合理的设计高性能乙醇燃料电池催化剂。选用高性能的PtRh/RGO催化剂,结合同位素示踪法和电化学原位红外光谱技术,研究了不同温度下乙醇的电氧化过程。循环伏安研究表明,乙醇电氧化性能及其C-C键断裂的程度为PtRh/RGO (45℃)>PtRh/RGO (25℃)>商业Pt/C。电化学原位红外光谱从分子水平跟踪了乙醇的电氧化过程,观察到随着电位的增加, CO2, CO,-CH3,-C-O特征峰的强度逐渐增加。CO2和CH3COOH分别归属于乙醇完全氧化和不完全氧化的终产物,因此红外光谱中两种物质特征峰积分面积的比值[CO2]/[CH3COOH]可做为CO2选择性的量度。用来定量标定CH3COOH的特征峰是位于1 280 cm-1的-C-O振动峰,但对于PtRh/RGO催化剂的红外光谱而言,它的乙酸特征峰振动峰位1 280 cm-1附近出现1 214 cm-1甲醇衍生物的振动峰,通过一种反射红外光谱与标样透射红外光谱差减扣除叠加峰方法,定量计算了叠加峰中1 280 cm-1特征峰的积分强度,从而计算出PtRh/RGO的CO2选择性。结果表明对比25℃时, 45℃下PtRh/RGO具有更高的选择性, 0.3 V时提高48.1%, 0.5和0.6 V时略有提高, 0.4 V时降低,这可能是乙醇中β-C和水中OH竞争吸附所致。在两种反应温度条件下, CO2选择性都在电位高于0.4 V时呈现下降趋势。为了进一步研究CO2来源于α-C或β-C的完全氧化,使用同位素标记的13CH312CH2OH做为探针分子,通过电化学原位红外光谱研究了25和45℃下PtRh/RGO电极上乙醇电氧化过程。结果表明,β-C完全氧化为CO2的起始电位与温度无关,都为0.3 V。通过用13CO2/12CO2积分面积的比值定量分析,发现45℃下,该比值在电位0.3~0.5 V时相比于25℃下分别增加0.11, 0.18和0.22,表明随着温度或电位的增加,β-C完全氧化的选择性增加。     

红外光谱分析技术在浮选过程中的应用研究进展

随着浮选研究的深入发展,以捕收剂为核心的浮选药剂作用机理的研究逐渐成为研究焦点。红外光谱以速度快、成本低、无损等特点成为浮选药剂作用机理研究最为重要的手段之一。首先从文献报道数量和比例说明红外光谱在该研究中的重要地位,并总结了常见浮选药剂的红外光谱特征,最后分别阐述了红外光谱在捕收剂、抑制剂、活化剂等浮选药剂作用机理中的应用研究进展。归纳出红外光谱用于判定捕收剂在矿物表面作用三种机制的判据： 如果捕收剂作用后的矿物表面有新的吸收峰,则捕收剂在矿物表面发生了化学反应;如果仅有吸收峰的位置发生移动,并超过测试设备本身误差范围的移动量,则捕收剂在矿物表面形成的是化学吸附;排除上述产生的新红外特征吸收峰和红外特征峰的移动,且通过反复水洗即可清除表面沾染的捕收剂分子,则捕收剂在矿物表面发生的是物理吸附。并指出红外光谱在浮选过程中的应用研究存在的两大问题,一是将捕收剂与矿物表面的化学反应和化学吸附机理混淆;二是忽视红外光谱仪器吸收峰位移2～4 cm-1背景误差。展望未来红外光谱在浮选过程中的应用研究应该着眼于多种药剂混合用药在矿物表面作用机理的研究,该领域内红外光谱的定量分析研究及红外光谱吸收峰位移的背景误差分析等三方面。     

DRIFTS study of Cu1Zr1Ce9Odelta catalysts for selective CO oxidation

The Cu1Zr1Ce9Odelta catalysts synthesized with coprecipitation method were used into the selective CO oxidation in hydrogen-rich gas. The adsorbed species and the intermediates on Cu1Zr1Ce9Odelta catalysts were examined by in-situ diffuse reflectance FTIR spectroscopy (in-situ DRIFTS) technique. It was found that hydrogen, oxygen and CO in the feed stream were adsorbed competitively at the same adsorption sites on the surface of Cu1Zr1Ce9Odelta catalysts. The pretreatment with hydrogen caused the deep reduction of Cu+ species to Cu0 species and decreased the capacity of CO adsorption on the catalyst surface. The Cu1Zr1Ce9Odelta catalyst pretreated with oxygen offered more active oxygen species and inhibited the deep reduction of Cu+ species. The helium pretreatment only purified the surface of Cu1Zr1Ce9Odelta catalyst. Two IR bands at 2938.7 and 2843.8 cm(-1) due to bridged formate and bidentate formate species appeared at 180 degrees C. The active oxygen anion of Cu1Zr1Ce9Odelta catalyst could react with CO and produce carbonate species at room temperatures. The carbonate and formate species occupied the adsorption sites and deteriorated the catalytic performance of Cu1Zr1Ce9Odelta. Flushing the Cu1ZnrCe9Odelta catalyst with helium at 300 degrees C, the bidentate formate species on the catalyst surface decomposed to monodentate carbonate species and then further decomposed to CO2, which could release the adsorption sites and restore well the catalytic activity.     

The adsorption of CO and oxygen on Cu layers on a W(110) surface

The adsorption of CO, and to a lesser extent that of oxygen on Cu layers deposited on a W(110) surface has been investigated by thermal desorption. Auger, and XPS measurements. For CO the amount adsorbed decreases monotonically with Cu thickness from 1–5 layers. For O there is a slight increase for 1 layer, followed by a steep decrease up to 4 Cu layers where the amount adsorbed levels off. CO adsorption shifts the core levels of Cu (observed for 1 layer of Cu) to higher binding energy by 0.4 eV; the O 1s level of CO is also shifted to higher binding energy by 1.5 eV, relative to CO/W(110) suggesting that electron transfer from CO occurs but is passed on to the underlying W. For O adsorption there is very little shift in the Cu core levels or in the O 1s level, relative to O/W(110). Thermal desorption of CO at saturation coverage from Cu/W(110) shows desorption peaks at 195, 227 and 266 K, as well as small peaks associated with CO desorption from clean W, namely a peak at 363 K and β-desorption peaks at 1080 and 1180 K. As CO coverage is decreased the 195 and 227 K peaks disappear successively; the W-like peaks remain unchanged in intensity. It is argued that the latter may be due to adsorption on bare W at domain boundaries of the Cu overlayer, while the 190–266 K peaks are associated with adsorption on Cu, but probably involve reconstruction of the Cu layer. For n = 2–8 a single but composite peak is seen, shifting from 180 to 150 K as Cu thickness increases as well as a minor peak at 278 K, which virtually vanishes on annealing the Cu deposit at 850 K. The effect of tungsten electronic structure on the behavior of adsorbates on the Cu overlayers, as well as similar effects in other snadwich systems are discussed.     

The adsorption of CO on clean and potassium promoted FeO surfaces

The adsorption of CO on a FeO (wustite) surface was investigated using UPS, AES and temperature programmed desorption. These results are compared to those obtained from the same sample following addition of potassium from the decomposition of KOH. CO adsorption was identified following exposure at 300 K to the potassium free surface. The adsorbed species readily desorbs below 500 K. CO adsorption was poisoned by pre-exposure to oxygen at 300 K. This suggests CO is adsorbed at surface oxygen vacancies. CO induced UPS emission features are different from those typically found for CO chemisorbed on transition metal surfaces. The presence of potassium alters the adsorption behavior of CO. The thermal desorption maximum shifts to 625 K. UPS results indicate molecular CO adsorption at 300 K and upon heating to 470 K CO dissociates. The presence of potassium thus promotes CO dissociation on FeO.     

DRIFTS study of different gas adsorption for CO selective oxidation on Cu-Zr-Ce-O catalysts

The adsorptions of different gases (CO, H₂ and O₂) in the hydrogen-rich gas on the co-precipitated Cu-Zr-Ce-O catalyst were discussed and the active sites were ascertained with infrared spectroscopy technique. It was shown that the adsorption strength of CO was stronger than that of O₂ or H₂. Hydrogen and CO were competitive adsorption and the coexistence H₂ and CO on the surface accelerated the rate of CO desorption. Adsorbed H₂ could convert into geminal OH groups on the ceria surface at high temperatures in the absence of oxygen, while it was easy to form surface hydroxyl groups at low temperatures and condensed to physical water with increasing desorption temperature in the existence of oxygen. The adsorption of CO₂ was strong and it could transform into thermal stable carbonate species even in the reaction conditions. The active sites of the Cu-Zr-Ce-O catalyst were Cu²⁺ and Cu⁺, mainly the latter. The oxygen defect sites could be formed on the Cu-Zr-Ce-O catalyst surface through dehydration and decarboxylation.     

二氧化锆相结构的漫反射光谱表征

利用紫外漫反射光谱考察了二氧化锆基催化剂的表面相组成 ,结合X射线粉末衍射、差热分析和X射线光电子能谱研究了铂化以及Al2 O3 的引入对样品中ZrO2 体相和表面相结构的影响。结果表明 :通氢还原铂化过程使部分的ZrO2 由四方相向单斜相转化 ,而且在催化剂表面这一效应更为显著。随着基体中引入Al2 O3 量的增加 ,二氧化锆的相变温度不同程度地向高温转移 ,添加Al2 O3 使ZrO2 得到较好的分散并抑制单斜相二氧化锆的生成。     

Application of thermal desorption methods in studies of catalysis: II. The oxidation of carbon monoxide on platinum

One of the major difficulties encountered in catalytic research has been the experimental characterization of the catalyst surface in its working state. Using thermal desorption techniques, we have developed a method capable of providing a quantitative measure of the concentrations of certain adsorbed reactants during catalysis. In a study of the oxidation of CO on polycrystalline platinum, three distinct reaction mechanisms have been distinguished: (1) the interaction of an oxygen molecule with a vacant Pt surface site and an adjacent adsorbed CO molecule forming a complex which dissociates to form a CO₂ molecule and an adsorbed oxygen atom; (2) the reaction between adsorbed CO and an adsorbed oxygen atom, a process in which surface transport is required to bring the reactants together; and (3) the reaction between a colliding CO molecule and an adsorbed oxygen atom. Rate constants for the reaction steps have been measured, and the active surface sites and reactive surface states on the Pt catalyst have been characterized in terms of the adsorption properties of CO.     

The coadsorption of CO and H2 on Fe(100)

The coadsorption of CO and hydrogen on an Fe(100) surface was studied by temperature programmed desorption and X-ray photoelectron spectroscopy. It was found that CO adsorption blocked the subsequent dissociative adsorption of H₂, although it did not seem to affect the hydrogen binding energy. Preadsorption of hydrogen was observed to reduce the binding energy of CO subsequently adsorbed and to inhibit the dissociation of CO. A new surface species was identified in a coadsorbed layer of CO and hydrogen. This species was evidenced by the formation of a desorption peak for H₂ at 475 K when CO was adsorbed subsequent to H₂ adsorption.     

Low-energy electron diffraction,Auger electron spectroscopy,and thermal desorption studies of chemisorbed CO and O2 on the (111) and stepped [6(111) × (100)] iridium surfaces

The adsorption of CO, O₂, and H₂O was studied on both the (111) and [6(111) × (100)] crystal faces of iridium. The techniques used were LEED, AES, and thermal desorption. Marked differences were found in surface structures and heats of adsorption on these crystal faces. Oxygen is adsorbed in a single bonding state on the (111) face. On the stepped iridium surface an additional bonding state with a higher heat of adsorption was detected which can be attributed to oxygen adsorbed at steps. On both (111) and stepped iridium crystal faces the adsorption of oxygen at room temperature produced a (2 × 1) surface structure. Two surface structures were found for CO adsorbed on Ir(111); a (√3 × √3)R30° at an exposure of 1.5–2.5 L and a (2√3 × 2√3)R30° at higher coverage. No indication for ordering of adsorbed CO was found on the Ir(S)-[6(111) × (100)] surface. No significant differences in thermal desorption spectra of CO were found on these two faces. H₂O is not adsorbed at 300 K on either iridium crystal face. The reaction of CO with O₂ was studied on Ir(111) and the results are discussed. The influence of steps on the adsorption behaviour of CO and O₂ on iridium and the correlation with the results found previously on the same platinum crystal faces are discussed.     

Nickel carbonyl adsorption on the Ni(111) surface

Overlayers formed by the adsorption of Ni(CO)₄ in CO on the Ni(111) surface at 100 K were characterized using high resolution electron energy loss spectroscopy and thermal desorption spectroscopy. At temperatures below 135 K, molecular nickel carbonyl adsorbs on the CO saturated Ni(111) surface as suggested by several observations. Vibrational transitions characteristic of molecular Ni(CO)₄ are dominant. The energy dependence of both the elastic and inelastic electron scattering cross sections are dramatically altered by Ni(CO)₄ adsorption. All of the mass spectrometer ionization fragments typical of molecular Ni(CO)₄ are observed in the narrow thermal desorption peak at 150 K. The inelastic scattering cross sections for both adsorbed nickel carbonyl and adsorbed CO on the Ni(111) surface suggest that a nonresonant dipole scattering mechanism is dominant.