RESUMO
The detailed potential energy surfaces (PESs) of poorly understood ion-molecule reactions of CH(3)O(-) with O(2)(X(3)Σ(g)(-)) and O(2)(a(1)Δ(g)) are accounted for by the density functional theory and ab initio of QCISD and CCSD(T) (single-point) theoretical levels with 6-311++G(d,p) and 6-311++G(3df,2pd) basis sets for the first time. For the reaction of CH(3)O(-) with O(2)(X(3)Σ(g)(-)) ((3)R), it is shown that a hydrogen-bonded complex (3)1 is initially formed on the triplet PES, which is 1.8 kcal/mol above reactants (3)R at the CCSD(T)//QCISD level, from which all the products P(1)-P(8) can be generated. As to the reaction of CH(3)O(-) with O(2)(a(1)Δ(g)) ((1)R), it is found that the two energetically low-lying complexes of (1)1(-31.5 kcal/mol) and (1)2(-24.1 kcal/mol) are initiated on the singlet PES. Starting from them, a total of seven products may be possible, that is, besides P(1), P(2), P(3), P(4), and P(8), which are the same as on the triplet PES, there exist also another two products, P(9) and P(10). For both reactions, taking the thermodynamics and kinetics into consideration, the hydride-transfer species P(1)(CH(2)O + HO(2)(-)) should be the most favorable product followed by P(8)(e + CH(2)O + HO(2)), which is a secondary product of electron-detachment from P(1), and the generation of endothermic P(7)(17.7 kcal/mol) for the reaction of CH(3)O(-) with O(2)(X(3)Σ(g)(-)) is also possible at high temperature, whereas the remaining products are negligible. The measured branching ratio of products for CH(3)O(-) with O(2)(X(3)Σ(g)(-)) by Midey et al. is 0.85:0.15 for P(1) and P(8), and that of CH(3)O(-) with O(2)(a(1)Δ(g)) is 0.52:0.48 with more P(8), which can be rationalized by our theoretical results that P(8) on the triplet PES is 4.9 kcal/mol above (3)R, whereas both P(1) and P(8) on the singlet PES are very low-lying at 45.6 and 25.2 kcal/mol below (1)R energetically. The measured total reaction rate constant of CH(3)O(-) with O(2)(a(1)Δ(g)) is k = 6.9 × 10(-10) cm(3) s(-1) at 300 K, which is larger than that of k = 1.1 × 10(-12) cm(3) s(-1) for the reaction of CH(3)O(-) with O(2)(X(3)Σ(g)(-)). This is understandable because both P(1) and P(8) on the singlet PES can be generated barrierlessly, whereas to give all the products on the triplet PES has to pass the barrier of (3)1(1.8 kcal/mol) at the CCSD(T)//QCISD level. It is expected that the present theoretical study may be helpful for understanding the reaction mechanisms related to CH(3)O(-) and even CH(3)S(-).
RESUMO
OBJECTIVE: To establish of acute respiratory distress syndrome (ARDS) model in canine after inhalation of perfluoroisobutylene (PFIB), and to observe the progressing of lung injury, and to study the mechanisms of injury. METHODS: A device of inhalation of PFIB for canine was made. The concentration of PFIB was 0.30 - 0.32 mg/L. Serum IL-6 and IL-8 were dynamically measured. Clinical manifestations, pathology of organs in canine were observed. RESULTS: (1) During inhalation, the concentration of PFIB remained stable; (2) After inhalation, blood arterial oxygen partial pressure fell gradually, and eventually met the criteria for diagnosing ARDS; (3) The level of IL-8 in serum rises significantly after inhalation (P < 0.05), whereas that of IL-6 was not obviously altered (P > 0.05); (4) Within 6 hours after inhalation, no abnormality in canine was observed, but afterwards symptoms gradually appeared, and typical breath of ARDS, such as high frequency and lower level could be seen in later phase; (5) Pathological examination showed severe congestion, edema and atelectasis in most part of both lungs, and signs of anoxia in other organs. CONCLUSIONS: (1) The device designed is capable of ensuring control of inhalation of PFIB; (2) Exposure to PFIB for 30 mins, canines all met the criteria for diagnosing ARDS 22 hours after inhalation, therefore the modeling is successful; (3) PFIB specifically damages the lung by causing excessive inflammation.