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CHCl3 |
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Chlorine and Deuterium |
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Nuclear
Quadrupole Coupling Constants |
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in Chloroform |
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35Cl nqcc's in
chloroform were first measured in 1967 by Wolf et al. [1], and
revisited in 1995 by Carpenter et al. [2]. In 2006,
Białkowska-Jaworska, et al. [3] determined the complete nqcc tensors
for both 35Cl and 37Cl.
An equilibrium structure has been derived by Colmont et al. [4]. |
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Chlorine nqcc tensors calculated here on the
equilibrium structure are compared with the experimental nqcc tensors [3] in Tables
1 - 3. The calculated deuterium nqcc is given in Table 4. Structure
parameters and atomic coordinates are given in Tables 5 and 6, respectively. |
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Calculation was made also on recently derived rm(2), reBO, and reSE structures [5]. These are summarized in Table 7. |
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In Table 1, Xuu is the component of the nqcc tensor along the
threefold symmetry axis. Corresponding to the atomic coordinates
given below in Table 6, Xvv and Xww are the components
along the v- and w- axes for the Cl atom in the uv-plane. Subscripts x,y,z refer to the principal
axes of the nqcc tensor. The y-axis is chosen coincident with the
w-axis. Ø (degrees) is the angle between its subscripted parameters.
ETA = (Xxx - Xyy)/Xzz. |
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In Tables 2 and 3, subscripts a,b,c refer to the principal axes of the inertia tensor; x,y,z to the principal
axes of the nqcc tensor. Ø (degrees) is the angle between its subscripted parameters.
ETA = (Xxx - Xyy)/Xzz. |
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RMS is the root mean square
difference between calculated and experimental diagonal nqcc's.
RSD is the residual standard deviation of calibration of the
model for calculation of the nqcc's. |
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Table 1. Chlorine nqcc's in CH35Cl3 (MHz). Calculation was made on the equilibrium structure of Colmont et al. [4]. The subscripts in parentheses are the axes labels of Ref. [3]. |
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Calc. |
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Expt. [3] |
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35Cl |
Xuu(cc) |
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28.62 |
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28.6436(4) |
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Xvv(aa) |
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67.89 |
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67.8309(5) |
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Xww(bb) |
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39.27 |
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39.1872(5) |
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Xuv(ac) |
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34.29 |
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34.137(32) |
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RMS |
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0.06 (0.13 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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39.57 |
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39.501(18) |
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Xyy |
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39.27 |
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39.1872(5) |
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Xzz |
- |
78.84 |
- |
78.688(18) |
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ETA |
- |
0.0038 |
- |
0.0040(2) |
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Øz,u(c) |
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72.30 |
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72.357(13) |
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Øu(c),CCl |
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71.77 |
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71.77(2) |
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Øz,CCl |
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0.53 |
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0.59(2) |
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Table 2. 37Cl nqcc's in CH37Cl35Cl2 (MHz). Calculation was made on the equilibrium structure of Colmont et al. [4]. |
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Calc. |
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Expt. [3] |
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37Cl |
Xcc |
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22.64 |
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22.6575(11) |
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Xaa |
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53.59 |
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53.5442(10) |
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Xbb |
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30.95 |
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30.8867(10) |
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Xac |
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26.91 |
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26.52(20) |
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RMS |
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0.04 (0.12 %) |
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RSD |
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0.44 (1.1 %) |
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Xxx |
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31.18 |
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30.98(11) |
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Xyy |
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30.95 |
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30.8867(10) |
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Xzz |
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62.13 |
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61.87(11) |
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ETA |
- |
0.0038 |
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0.0015(19) |
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Øz,c |
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72.39 |
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Øc,C37Cl |
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71.86 |
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Øz,C37Cl |
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0.53 |
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Table 3. 35Cl nqcc's in CH37Cl35Cl2 (MHz). Calculation was made on the equilibrium structure of Colmont et al. [4]. |
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Calc. |
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Expt. [3] |
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35Cl |
Xcc |
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28.57 |
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28.5890(6) |
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Xaa |
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12.53 |
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12.4880(7) |
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Xbb |
- |
41.10 |
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41.0770(7) |
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Xab |
± |
46.35 |
± |
46.2901(66) |
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Xac |
- |
17.17 |
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17.15(15) |
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Xbc |
± |
29.77 |
± |
29.665(88) |
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RMS |
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0.03 (0.11 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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39.57 |
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39.534(76) |
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Xyy |
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39.27 |
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39.182(25) |
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Xzz |
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78.84 |
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78.716(62) |
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ETA |
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0.0038 |
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0.0045(10) |
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Øz,C35Cl |
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0.53 |
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Table 4. Deuterium nqcc's in CHCl3 (kHz). |
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Calc. |
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Expt. |
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2H |
Xzz |
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182.7 |
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Table 5. Structure parameters, re [4] (Å and degrees). |
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CCl |
1.760 |
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CH |
1.080 |
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HCCl |
108.23 |
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ClCCl |
110.68 |
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Table 6. CH35Cl3. Atomic coordinates, re |
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c//u (Å) |
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a//v (Å) |
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b//w (Å) |
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Cl |
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0.0700 |
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1.6717 |
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0.0 |
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Cl |
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0.0700 |
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0.8358 |
± |
1.4477 |
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C |
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0.4806 |
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0.0 |
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0.0 |
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H |
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1.5606 |
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0.0 |
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0.0 |
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Table 7. Molecular structure parameters (Å and degrees) [5] and 35Cl nqcc's in CH35Cl3 (MHz). RMS is the root mean sqaure difference between calculated and experimental (see Table 1) diagonal nqcc's. |
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rm(2) |
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reBO |
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reSE |
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CCl |
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1.7544(7) |
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1.7592 |
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1.7595(1) |
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CH |
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1.0800(24) |
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1.0806 |
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1.0818(6) |
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HCCl |
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107.43(8) |
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107.934 |
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108.080(16) |
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ClCCl |
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111.43(8) |
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110.964 |
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110.825(16) |
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Xuu |
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30.01 |
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29.19 |
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28.91 |
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Xvv |
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69.02 |
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68.39 |
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68.14 |
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Xww |
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39.01 |
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39.20 |
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39.23 |
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|Xuv| |
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32.10 |
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33.50 |
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33.90 |
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RMS |
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1.05 (2.3 %) |
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0.45 (1.0 %) |
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0.24 (0.5 %) |
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[1] A.A.Wolf, Q.Williams, and T.L.Weatherly, J.Chem.Phys.
47,5101(1967). |
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[2] J.H.Carpenter, P.J.Seo, and D.H.Whiffen, J.Mol.Spectrosc.
170,215(1995). |
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[3] E.Białkowska-Jaworska, Z.Kisiel, and L.Pszczółkowski, J.Mol.Spectrosc. 238,72(2006). |
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[4] J.M.Colmont, D.Priem, P.Dréan, J.Demaison, and
J.E.Boggs, J.Mol. Spectrosc. 191,158(1998). |
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[5] J.Demaison, J.Mol.Spectrosc. 251,217(2008). |
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Related ... |
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"Theoretical Investigation of the Nuclear Quadrupole
Interaction of CH3Cl, CH2Cl2 and CHCl3"
G.Frantz, H.Dufner, and P.C.Schmidt, Z.Naturforsch. 49a,116(1993). |
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CFCl3 |
SiHCl3 |
CH3CCl3 |
OPCl3 |
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NCl3 |
PCl3 |
AsCl3 |
SPCl3 |
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CH3Cl |
CH2Cl2 |
CH3D |
CDF3 |
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Table of Contents |
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Molecules/Chlorine |
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Molecules/Deuterium |
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Summary/Methyls
Deuterium nqcc's in the substituted methanes. |
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CHCl3.html |
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Last
Modified 30 April 2008 |
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