Li Lok Hin Desmond, Douglas Kevin M, Hall Ffion, Kirker Alice, Driver Luke, de Boer Gregory N, Kapur Nikil, Lehman Julia H, Blitz Mark A, Heard Dwayne E
School of Chemistry, University of Leeds, Leeds LS2 9JT, U.K.
EPSRC CDT in Fluid Dynamics, School of Computing, University of Leeds, Leeds LS2 9JT, U.K.
J Phys Chem A. 2025 Jul 17;129(28):6289-6305. doi: 10.1021/acs.jpca.5c03008. Epub 2025 Jul 1.
The kinetics of the dimerization of NH in helium and nitrogen bath gas within the supersonic flow of a Laval nozzle were investigated at very low temperatures. Experimentally, the fraction of the NH monomer, , remaining in the flow at 91 K in N and at 35 K in He for a total bath gas density [M]∼5 × 10 molecules cm was monitored using fluorescence from the electronically excited NH photofragment formed following NH photolysis at 213 nm. No dimerization was observed up to [NH] = 1 × 10 molecules cm for 160 mm downstream of the 91 K N nozzle, nor up to [NH] = 5 × 10 molecules cm for 150 mm downstream of the 35 K He nozzle. Dimerization was observed at higher [NH], being more pronounced at lower temperatures. For the C and C conformers of the NH dimer, calculations at the CCSD(T)/aug-cc-pVTZ level gave a zero-point vibrational-energy corrected binding energy of -7.52 and -7.33 kJ mol, respectively. Energy-grained master equation calculations based on statistical rate theory using the open-source MESMER package were used to calculate rate coefficients for dimerization, , over the temperature range = 25-300 K and [M] = 10-10 molecules cm for He and N. displayed a negative dependence and a positive [M] dependence and was found to be sensitive to changes in the low-lying vibrational frequencies of the NH dimer, for example, the inclusion of a hindered rotor potential for the internal twisting mode, which alters the density of states. Using the axial profiles of , [M], and velocity for the Laval nozzles, the calculated values of were used to calculate in the flow for comparison with the experiment. At higher [NH], when dimerization was observed, the calculations significantly underestimated the degree of dimerization taking place in the flow, with a significant increase in the calculated value of required to match the experiment. The reasons for the discrepancy are discussed, for example, errors in the calculation of the density of states for the NH dimer and the average energy removed per collision by the bath gas at very low temperatures.
在非常低的温度下,研究了拉瓦尔喷管超音速流中氦气和氮气浴气中NH二聚化的动力学。实验上,利用213nm处NH光解后形成的电子激发NH光碎片的荧光,监测了在91K的氮气和35K的氦气中,对于总浴气密度[M]∼5×10分子/cm³,流中剩余的NH单体的分数。在91K氮气喷管下游160mm处,[NH] = 1×10分子/cm³时未观察到二聚化,在35K氦气喷管下游150mm处,[NH] = 5×10分子/cm³时也未观察到二聚化。在较高的[NH]时观察到二聚化,在较低温度下更明显。对于NH二聚体的C和C构象,在CCSD(T)/aug-cc-pVTZ水平上的计算给出了零点振动能校正的结合能分别为-7.52和-7.33kJ/mol。基于统计速率理论,使用开源MESMER软件包进行的能量分辨主方程计算,用于计算在25-300K温度范围和[M] = 10-10分子/cm³的氦气和氮气中二聚化的速率系数。显示出负的依赖性和正的[M]依赖性,并且发现对NH二聚体的低振动频率的变化敏感,例如,包含内部扭转模式的受阻转子势,这会改变态密度。利用拉瓦尔喷管的轴向分布、[M]和速度,计算得到的值用于计算流中的,以便与实验进行比较。在较高的[NH]时,当观察到二聚化时,计算结果显著低估了流中发生的二聚化程度,需要显著增加计算得到的值才能与实验匹配。讨论了差异的原因,例如,NH二聚体态密度计算中的误差以及在非常低的温度下浴气每次碰撞去除的平均能量。