Armentrout Peter B, Sweeney Andrew F
Department of Chemistry, University of Utah, 315 South 1400 East, Rm 2020, Salt Lake City, Utah 84112, United States.
Eur J Mass Spectrom (Chichester). 2015;21(3):497-516. doi: 10.1255/ejms.1334.
Cross sections for the threshold collision-induced dissociation of Cu(2+)(H(2)O)(n), where n = 8 - 10, are measured using a guided ion beam tandem mass spectrometer. The primary dissociation pathway is found to be loss of a single water molecule followed by the sequential loss of additional water molecules until n = 8, at which point charge separation to form CuOH(+)(H(2)O)(4) (+) H(+)(H(2)O)(3) is observed to occur at a slightly lower energy than loss of a water molecule. Competition from charge separation prohibits the formation of appreciable amounts of the n = 7 or smaller complexes as reactants in the source. These findings indicate that Cu(2+) has a critical size of 8. Analysis of the data using statistical modeling techniques that account for energy distributions and lifetime effects yields primary and sequential bond dissociation energies (BDEs) for loss of one and two water molecules from n = 8 - 10 complexes as well as the barrier for charge separation from n = 8. More speculative analysis extends the thermochemistry obtained down to n = 5 and 6. Theoretical BDEs are determined from quantum chemical calculations using structures optimized at the B3LYP/6 311(+)G(d,p) level along with the lowest-energy isomers suggested by single point energies at the MP2(full), M06, B3LYP, and B3P86 levels of theory using a 6- 311(+)G(2d,2p) basis set. BDEs at 0K are converted to 298 K thermodynamic values using a rigid rotor/harmonic oscillator approximation. Experimental and theoretical entropies of activation suggest that a third solvent shell forms at n = 9, in accord with previous findings. The present work represents the first experimentally determined hydration enthalpies for the Cu(2+)(H(2)O)n system.
使用导向离子束串联质谱仪测量了Cu(2+)(H(2)O)(n)(n = 8 - 10)阈值碰撞诱导解离的截面。发现主要解离途径是先失去一个水分子,然后依次失去更多水分子,直到n = 8,此时观察到电荷分离形成CuOH(+)(H(2)O)(4) (+) H(+)(H(2)O)(3),其发生能量略低于失去一个水分子的能量。电荷分离的竞争阻止了源中形成可观量的n = 7或更小的络合物作为反应物。这些发现表明Cu(2+)的临界尺寸为8。使用考虑能量分布和寿命效应的统计建模技术对数据进行分析,得出了n = 8 - 10络合物失去一个和两个水分子的一级和连续键解离能(BDE)以及n = 8电荷分离的势垒。更具推测性的分析将获得的热化学延伸到n = 5和6。理论BDE通过量子化学计算确定,使用在B3LYP/6 311(+)G(d,p)水平优化的结构,以及在MP2(full)、M06、B3LYP和B3P86理论水平使用6- 311(+)G(2d,2p)基组的单点能量建议的最低能量异构体。使用刚性转子/谐振子近似将0K时的BDE转换为298K热力学值。实验和理论活化熵表明,在n = 9时形成了第三溶剂壳,这与先前的发现一致。本工作代表了首次通过实验确定的Cu(2+)(H(2)O)n系统的水合焓。