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CH3ClC=CH2 |
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Chlorine |
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Nuclear
Quadrupole Coupling Constants |
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in 2-Chloropropene |
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Calculation of the chlorine nqcc's in
2-chloropropene was made on a molecular structure derived ab initio,
as described below. Earlier
measurements of the nqcc's were made by Good et al. [2] and Unland et
al. [3]. The calculated nqcc's are compared with the experimental
results of Fliege and Dreizler [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 2-Chloropropene (MHz). |
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Calc. |
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Expt. [1] |
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35Cl |
Xaa |
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68.36 |
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68.072 |
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Xbb |
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37.84 |
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37.097 |
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Xcc |
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30.51 |
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30.975 |
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|Xab| |
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9.73 |
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RMS |
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0.53 (1.2 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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38.73 |
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37.99 * |
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Xyy |
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30.51 |
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30.975 |
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Xzz |
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69.24 |
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68.96 |
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ETA |
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0.119 |
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0.102 |
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Øz,a |
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5.19 |
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5.24 |
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Øa,CCl |
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5.00 |
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5.00 |
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Øz,CCl |
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0.19 |
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0.24 |
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37Cl |
Xaa |
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53.90 |
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53.763 |
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Xbb |
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29.86 |
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29.370 |
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Xcc |
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24.05 |
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24.394 |
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|Xab| |
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7.94 |
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RMS |
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0.36 (0.99 %) |
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RSD |
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0.44 (1.1 %) |
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* Calculated here from the experimental
diagonal nqcc's and the calculated off-diagonal nqcc. |
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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.[4]. 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.[5].
The CH bond lengths were corrected using r = 1.001 ropt,
where
ropt is obtained by MP2/6-31G(d,p) optimization [6].
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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Cl |
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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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H |
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 = 1.740 |
A3 = 114.14 |
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R2 = 1.491 |
A4 = 120.15 |
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R3 = 1.330 |
A5 = 121.87 |
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R4 = 1.080 |
A6 = 119.34 |
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R5 = 1.081 |
A7 = 110.08 |
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R6 = 1.089 |
A8 = 110.38 |
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R7 = 1.090 |
D = 120.49 |
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| Table 3. Rotational Constants (MHz). 35Cl
species. |
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Calc. ropt |
Expt. [1] |
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A |
9 380.8 |
9 271.706(79) |
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B |
4 985.9 |
4 983.816(45) |
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C |
3 322.4 |
3 304.414(45) |
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[1] E.Fliege and H.Dreizler,
Z.Naturforsch. 38a,1231(1983). |
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[2] W.Good, R.J.Conan Jr., A.Bauder, and
Hs.H.Günthard, J.Mol.Spectrosc. 41,381(1972). |
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[3] M.L.Unland, V.Weiss, and W.H.Flygare,
J.Chem.Phys. 42,2138(1965). |
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[4] J.Demaison, J.Cosléou, R.Bocquet,
and A.G.Lesarri, J.Mol.Spectrosc. 167,400(1994). |
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[5] I.Merke, L.Poteau, G.Wlodarczak, A.Bouddou,
and J.Demaison, J.Mol.Spectrosc. 177,232(1996). |
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[6] 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 |
CH2ClHC=CH2 |
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c-CH3FC=CHCl |
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Table of Contents |
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Molecules/Chlorine |
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2ClPropene.html |
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Last
Modified 21 June 2004 |
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