计算物理 ›› 2023, Vol. 40 ›› Issue (6): 712-717.DOI: 10.19596/j.cnki.1001-246x.8686
唐静1(), 张昕阳1, 江一航1, 金鑫1, 刘玉柱1,2,*(
)
收稿日期:
2022-12-26
出版日期:
2023-11-25
发布日期:
2024-01-22
通讯作者:
刘玉柱
作者简介:
唐静, 女, 主要从事光学和光谱的研究, E-mail: 202183430060@nuist.edu.cn
基金资助:
Jing TANG1(), Xinyang ZHANG1, Yihang JIANG1, Xin JIN1, Yuzhu LIU1,2,*(
)
Received:
2022-12-26
Online:
2023-11-25
Published:
2024-01-22
Contact:
Yuzhu LIU
摘要:
选择B3LYP计算方法, 使用6-311G ++(d, p)基组, 计算在外加电场(0~10.28 V·nm-1)作用下氯乙烷分子的结构特征和解离特性。计算结果表明: 随着电场强度增大, 分子的总能量增大, 碳碳单键键长呈减小趋势, 碳氯单键键长呈增大趋势, 偶极矩逐渐增大, 能隙先增大后减小, 红外吸收峰在不同频率下分别发生红移和蓝移, 拉曼峰强度变化。随着外电场增大, 势垒逐渐降低, 当外电场达到18.00 V·nm-1时, 势垒几乎消失, 实现电场降解。
中图分类号:
唐静, 张昕阳, 江一航, 金鑫, 刘玉柱. 氯乙烷在外电场中的解离性质[J]. 计算物理, 2023, 40(6): 712-717.
Jing TANG, Xinyang ZHANG, Yihang JIANG, Xin JIN, Yuzhu LIU. Study on Dissociation Properties of Chloroethane Under External Electric Field[J]. Chinese Journal of Computational Physics, 2023, 40(6): 712-717.
Method | DFT B3LYP 6-311G ++(d,p) | DFT B3LYP 6-311G | DFT B3LYP 6-31G | DFT B3LYP 3-21G | DFT B3LYP 3-21G +* | Exp.[ |
R1, 2/nm | 0.151 6 | 0.150 9 | 0.151 2 | 0.152 0 | 0.152 6 | 0.151 0 |
R2, 8/nm | 0.182 4 | 0.188 5 | 0.188 5 | 0.191 7 | 0.182 0 | 0.178 9 |
R1, 4/nm | 0.109 2 | 0.107 9 | 0.108 1 | 0.109 3 | 0.108 2 | 0.108 9 |
R2 | 0.999 593 872 | 0.997 035 708 | 0.997 064 748 | 0.994 823 484 | 0.999 546 143 |
表1 不同基组和方法优化后的氯乙烷分子的基态结构和实验值
Table 1 The ground state structure of CH3CH2Cl molecule optimized by different basis sets and methods with experimental value
Method | DFT B3LYP 6-311G ++(d,p) | DFT B3LYP 6-311G | DFT B3LYP 6-31G | DFT B3LYP 3-21G | DFT B3LYP 3-21G +* | Exp.[ |
R1, 2/nm | 0.151 6 | 0.150 9 | 0.151 2 | 0.152 0 | 0.152 6 | 0.151 0 |
R2, 8/nm | 0.182 4 | 0.188 5 | 0.188 5 | 0.191 7 | 0.182 0 | 0.178 9 |
R1, 4/nm | 0.109 2 | 0.107 9 | 0.108 1 | 0.109 3 | 0.108 2 | 0.108 9 |
R2 | 0.999 593 872 | 0.997 035 708 | 0.997 064 748 | 0.994 823 484 | 0.999 546 143 |
图1 氯乙烷分子基态稳定结构(其中箭头表示外加电场方向。)
Fig.1 Stable structure of the ground state of CH3CH2Cl molecule (The arrow indicates the direction of the external electric field.)
Method | DFT B3LYP 6-311G ++(d,p) | Exp.[ |
R1, 3/nm | 0.109 5 | 0.109 0 |
R1, 5/nm | 0.109 1 | 0.109 0 |
R2, 6/nm | 0.108 9 | 0.108 6 |
R2, 7/nm | 0.108 9 | 0.108 6 |
∠C1C2Cl | 112.18 | 111.02 |
∠H4C1C2 | 111.20 | 110.53 |
∠H3C1C2 | 109.28 | 109.30 |
∠H7C2C1 | 112.18 | 111.81 |
∠H4C1H5 | 108.48 | 108.26 |
∠H6C2H7 | 109.14 | 108.99 |
表2 氯乙烷分子键长和键角的理论值和实验值
Table 2 The theoretical value and experimental value of bond length and bond angle
Method | DFT B3LYP 6-311G ++(d,p) | Exp.[ |
R1, 3/nm | 0.109 5 | 0.109 0 |
R1, 5/nm | 0.109 1 | 0.109 0 |
R2, 6/nm | 0.108 9 | 0.108 6 |
R2, 7/nm | 0.108 9 | 0.108 6 |
∠C1C2Cl | 112.18 | 111.02 |
∠H4C1C2 | 111.20 | 110.53 |
∠H3C1C2 | 109.28 | 109.30 |
∠H7C2C1 | 112.18 | 111.81 |
∠H4C1H5 | 108.48 | 108.26 |
∠H6C2H7 | 109.14 | 108.99 |
图8 氯乙烷分子碳氯单键在不同电场下的单点扫描势能
Fig.8 Single point scanning potential energy of carbon-chlorine single bond of CH3CH2Cl molecule under different electric fields
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