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3,3-Bis(4-bromophenylsulfanyl)-1-methylpiperidin-2-one | 1448012-87-0

中文名称
——
中文别名
——
英文名称
3,3-Bis(4-bromophenylsulfanyl)-1-methylpiperidin-2-one
英文别名
3,3-bis[(4-bromophenyl)sulfanyl]-1-methylpiperidin-2-one
3,3-Bis(4-bromophenylsulfanyl)-1-methylpiperidin-2-one化学式
CAS
1448012-87-0
化学式
C18H17Br2NOS2
mdl
——
分子量
487.279
InChiKey
XTTBIHKEHSCAOR-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    6
  • 重原子数:
    24
  • 可旋转键数:
    4
  • 环数:
    3.0
  • sp3杂化的碳原子比例:
    0.28
  • 拓扑面积:
    70.9
  • 氢给体数:
    0
  • 氢受体数:
    3

反应信息

  • 作为产物:
    描述:
    1-甲基-2-哌啶酮4-二溴苯基二硫化物六甲基磷酰三胺正丁基锂二异丙胺 作用下, 以 四氢呋喃 为溶剂, 反应 3.33h, 以0.4 g的产率得到3,3-Bis(4-bromophenylsulfanyl)-1-methylpiperidin-2-one
    参考文献:
    名称:
    Conformational preferences for some 3,3-bis[(4′-substituted phenylsulfanyl)]1-methyl-2-piperidinones through spectroscopic and theoretical studies
    摘要:
    The analysis of the IR carbonyl band of some 3,3-bis[(4'-substituted phenylsulfanyl)]1-methyl-2-piperidinones 1-5 bearing as substituentsOMe1, Me2, H3, Cl4 and Br5, supported by B3LYP/6-31G(d,p) calculations for 3, indicated the existence of three conformers in the gas phase and practically a single conformer in solution. In the gas phase, the c(1) conformer is less polar and slightly more stable than the most polar c(2) conformer. The c(3) conformer is the least polar and least stable conformer. The summing up of the selected natural bond orbital delocalization orbital energies is practically the same (ca.136 kcal mol(-1)) for the c(1), c(2) and c(3) conformers of 3. Therefore, the trend of the [O delta- (CO)(center dot center dot center dot H delta+) o-Ph] (hydrogen bond) attractive electrostatic interactions along with the trend of the [O delta- (CO)S-center dot center dot center dot(delta-)] repulsive electrostatic interactions are the main factors which determine the observed computed relative populations for the c(1) (44%), c(2) (31%) and c(3) (25%) conformers. Moreover, the IR single carbonyl stretching band found (for 1-5) in solvents of increasing relative permissivity (CCl4, CHCl3, CH2Cl2, CH3CN), in agreement with polarisable continuum model calculations (for 3), show that the most polar c(2) conformer is practically unique in the solution (for 1-5), and the geometry is very close to that of the c(2') conformer in the solid state (for 1-4).[GRAPHICS].
    DOI:
    10.1080/17415993.2013.771359
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文献信息

  • Conformational preferences for some 3,3-bis[(4′-substituted phenylsulfanyl)]1-methyl-2-piperidinones through spectroscopic and theoretical studies
    作者:Paulo R. Olivato、Carlos R. Cerqueira Jr、Bruna Contieri、Jean M. M. Santos、Julio Zukerman-Schpector
    DOI:10.1080/17415993.2013.771359
    日期:2013.12.1
    The analysis of the IR carbonyl band of some 3,3-bis[(4'-substituted phenylsulfanyl)]1-methyl-2-piperidinones 1-5 bearing as substituentsOMe1, Me2, H3, Cl4 and Br5, supported by B3LYP/6-31G(d,p) calculations for 3, indicated the existence of three conformers in the gas phase and practically a single conformer in solution. In the gas phase, the c(1) conformer is less polar and slightly more stable than the most polar c(2) conformer. The c(3) conformer is the least polar and least stable conformer. The summing up of the selected natural bond orbital delocalization orbital energies is practically the same (ca.136 kcal mol(-1)) for the c(1), c(2) and c(3) conformers of 3. Therefore, the trend of the [O delta- (CO)(center dot center dot center dot H delta+) o-Ph] (hydrogen bond) attractive electrostatic interactions along with the trend of the [O delta- (CO)S-center dot center dot center dot(delta-)] repulsive electrostatic interactions are the main factors which determine the observed computed relative populations for the c(1) (44%), c(2) (31%) and c(3) (25%) conformers. Moreover, the IR single carbonyl stretching band found (for 1-5) in solvents of increasing relative permissivity (CCl4, CHCl3, CH2Cl2, CH3CN), in agreement with polarisable continuum model calculations (for 3), show that the most polar c(2) conformer is practically unique in the solution (for 1-5), and the geometry is very close to that of the c(2') conformer in the solid state (for 1-4).[GRAPHICS].
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