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CH3FC=CHCl |
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PDF |
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Chlorine |
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Nuclear
Quadrupole Coupling Constants |
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in cis-1-Chloro-2-Fluoropropene
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Calculation of the
chlorine nqcc's in cis-1-chloro-2-fluoropropene (Cl and F
are cis) was made on a molecular structure derived ab
initio, as described below. These are compared
with the experimental nqcc's of Stone et al. [1] in Table 1. Structure parameters are given
in Z-matrix format in Table 2. Rotational constants are given
in Table 3. |
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In Table 1, RMS is the root mean square difference
between calculated and experimental diagonal nqcc's (percentage of the
average of the magnitudes of the experimental nqcc's). RSD is the
calibration residual standard deviation for the B1LYP/TZV(3df,2p) model
for calculation of the chlorine nqcc's. |
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Subscripts a,b,c refer to the
principal axes of the inertia tensor; x,y,z to the principal axes
of the nqcc tensor. The nqcc y-axis is chosen coincident with the
inertia c-axis, these are perpendicular to the molecular symmetry plane.
Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
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Table 1. Chlorine
nqcc's in c-1-Chloro-2-Fluoropropene (MHz). |
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Calc. |
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Expt. [1] |
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35Cl |
Xaa |
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53.13 |
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53.09(20) |
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Xbb |
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20.03 |
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19.45(5) |
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Xcc |
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33.10 |
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33.64(20) |
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|Xab| |
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44.24 |
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43.5(30) |
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RMS |
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0.46 (1.3 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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40.86 |
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39.84 |
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Xyy |
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33.10 |
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33.64 |
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Xzz |
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73.96 |
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73.49 |
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ETA |
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0.105 |
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0.0844 |
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Øz,a |
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25.21 |
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Øa,CCl |
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25.94 |
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Øz,CCl |
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0.73 |
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37Cl |
Xaa |
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41.84 |
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41.70(20) |
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Xbb |
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15.75 |
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15.17(20) |
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Xcc |
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26.08 |
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26.53(20) |
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|Xab| |
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34.90 |
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RMS |
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0.43 (1.6 %) |
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RSD |
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0.44 (1.1 %) |
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Molecular Structure |
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The molecular structure
was optimized at the MP2/6-311+G(d,p) level of theory assuming
Cs symmetry. The optimized CC bond lengths, single
and double, were corrected using equations obtained from linear
regression analysis of the data given in Table IX of Ref.[2]. The
optimized CF bond lengths were corrected by regression analysis of the
data given in Table VI of Ref.[3]. For the CCl bond, the structure
was optimized at the MP2/6-311+G(2d,p) level and corrected by linear
regression analysis of the data given in Table 4 of Ref.[4]. The
CH bond lengths were corrected using r = 1.001 ropt, where
ropt is obtained by MP2/6-31G(d,p) optimization [5]. Interatomic
angles used in the calculation are those given by MP2/6-311+G(d,p)
optimization. |
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Table 2. Z-Matrix (Å and degrees). |
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F |
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C |
1 |
R1 |
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C |
2 |
R2 |
1 |
A3 |
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C |
2 |
R3 |
1 |
A4 |
3 |
180. |
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Cl |
4 |
R4 |
2 |
A5 |
3 |
180. |
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H |
4 |
R5 |
2 |
A6 |
3 |
0. |
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H |
3 |
R6 |
2 |
A7 |
6 |
0. |
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H |
3 |
R7 |
2 |
A8 |
6 |
-D |
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H |
3 |
R7 |
2 |
A8 |
6 |
D |
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R1 = 1.341 |
A3 = 113.39 |
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R2 = 1.483 |
A4 = 120.19 |
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R3 = 1.329 |
A5 = 123.42 |
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R4 = 1.713 |
A6 = 120.56 |
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R5 = 1.078 |
A7 = 110.48 |
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R6 = 1.088 |
A8 = 110.03 |
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R7 = 1.0905 |
D = 120.48 |
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Table 3. Rotational Constants (MHz). 35Cl
species. |
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Calc. ropt |
Expt. [1] |
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A |
9 989.6 |
9 958.22(5) |
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B |
2 288.9 |
2 285.88(2) |
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C |
1 884.0 |
1 879.89(2) |
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[1] R.G.Stone, S.L.Srivastava,
and W.H.Flygare, J.Chem.Phys. 48,1890(1968). |
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[2] J.Demaison, J.Cosléou, R.Bocquet,
and A.G.Lesarri, J.Mol.Spectrosc. 167,400(1994). |
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[3] R.M.Villamañan, W.D.Chen, G.Wlodarczak,
J.Demaison, A.G.Lesarri, J.C.López, and J.L.Alonso, J.Mol.Spectrosc.
171,223(1995) |
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[4] I.Merke, L.Poteau, G.Wlodarczak, A.Bouddou,
and J.Demaison, J.Mol.Spectrosc. 177,232(1996). |
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[5] J.Demaison and G.Wlodarczak, Structural
Chem. 5,57(1994). |
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H2C=CHCl |
H2C=CFCl |
c-ClHC=CHCl
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c-FHC=CHCl |
t-FHC=CHCl |
H2C=CCl2 |
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H2C=CClCN |
F2C=CHCl |
F2C=CCl2 |
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(CH3)2C=CHCl |
Cl2C=CHCl |
F2C=CFCl |
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c-CH3HC=CHCl |
t-CH3HC=CHCl |
CH3ClC=CH2 |
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CH2ClHC=CH2 |
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Table of Contents |
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Molecules/Chlorine |
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cCH3FCCHCl.html |
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Last
Modified 22 June 2004 |
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