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Individual Heat of Adsorption of Adsorbed CO Species on Palladium and Pd-Sn Nanoparticles Supported on Al2O3 by Using Temperature-Programmed Adsorption Equilibrium Methods

机译:程序升温吸附平衡法在Al2O3负载的钯和Pd-Sn纳米颗粒上吸附CO物种的单个吸附热

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The present article is dedicated to the adsorption of CO on reduced 2% Pd/Al2O3 and 2% Pd-x% Sn/Al2O3 (weight %, x = 2 or 5 wt %) in the 300-713 K temperature range to study the geometric and electronic effects of Sn on the palladium adsorption sites. Using Fourier transform infrared (FTIR) spectroscopy, it is shown that the insertion of Sn leads to (a) the total disappearance of the Pd sites forming bridged CO species (denoted as "B"), which are the dominant species on Pd-0 particles and (b) a significant increase in the Pd sites forming linear CO species (denoted as "L"). This is ascribed to a geometric effect of Sn that dilutes the superficial palladium sites. The measurement of the individual heats of adsorption of the different adsorbed CO species by using two original temperature-programmed adsorption equilibrium methods (denoted AEIR and TPAE) allows the estimation of the electronic effect of Sn on the Pd sites. On 2% Pd/Al2O3, in parallel to the formation of two strongly adsorbed B CO species, two linear L1(pd0) and L2(pd0) CO species are formed, which exhibit different heats of adsorption. For the dominant L1(pd0) CO species, the heat of adsorption decreases linearly, from 92 kJ/mol to 54 kJ/mol, as its coverage increases at coverage 0 and 1, respectively, while that of the L2(pd0) species is >165 kJ/mot at coverage 1. On the two Pd-Sn containing particles, two linear CO species are formed denoted L1(2pd-xSn) and L2(2Pd-xSn) with x = 2 or 5. The L1(2pd-xSn) species dominates the CO adsorption on the two solids. It is shown that its heat of adsorption (which is slightly dependent on x) linearly varies with its coverage: similar to 90 kJ/mol and similar to 50 kJ/mol at low and high coverage, respectively. The comparison with the heat of adsorption of L1(pd0) indicates that the electronic effect of tin is very modest, compared to its geometric effect. This conclusion is consistent with literature data dedicated to DFT calculation. Moreover, (a) XRD and TEM/EDX analysis suggest that bimetallic particles such as Pd3Sn and Pd2Sn are present and (b) the impact of tin on the H-2 chemisorption on Pd-0 sites are presented.
机译:本文致力于在300-713 K的温度范围内将CO吸附在还原的2%Pd / Al2O3和2%Pd-x%Sn / Al2O3(重量%,x = 2或5 wt%)上的研究方法。 Sn对钯吸附位点的几何和电子效应。使用傅里叶变换红外(FTIR)光谱,表明Sn的插入导致(a)形成桥接CO物种(表示为“ B”)的Pd位完全消失,这是Pd-0上的主要物种。 (b)形成线性CO物种(称为“ L”)的Pd位明显增加。这归因于锡的几何效应,稀释了表面钯位。通过使用两种原始的程序升温吸附平衡方法(表示为AEIR和TPAE)对不同吸附的CO物种的单个吸附热进行测量,可以估算Sn对Pd位的电子效应。在2%Pd / Al2O3上,平行于两种强烈吸附的B CO物质的形成,形成了两种线性的L1(pd0)和L2(pd0)CO物质,它们表现出不同的吸附热。对于主要的L1(pd0)CO物种,随着其覆盖率分别在覆盖率0和1处增加,吸附热从92 kJ / mol线性降低至54 kJ / mol,而L2(pd0)物种的吸附热则呈线性下降。在覆盖率1时> 165 kJ / mot。在两个含Pd-Sn的粒子上,形成了两个线性CO物种,分别表示为L1(2pd-xSn)和L2(2Pd-xSn),x = 2或5。L1(2pd- xSn)物种主导了两种固体对CO的吸附。结果表明,其吸附热(略微取决于x)随覆盖率呈线性变化:低覆盖率和高覆盖率分别接近90 kJ / mol和50 kJ / mol。与L1(pd0)的吸附热的比较表明,与锡的几何效应相比,锡的电子效应非常适中。该结论与专门用于DFT计算的文献数据一致。此外,(a)XRD和TEM / EDX分析表明存在双金属颗粒,例如Pd3Sn和Pd2Sn,(b)锡对Pd-0位点上H-2化学吸附的影响也存在。

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