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(CH3)2C=CHCl |
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Chlorine |
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Nuclear
Quadrupole Coupling Constants |
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in 1-Chloro-2-Methylpropene |
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Calculation of the chlorine
nqcc's in 1-chloro-2-methylpropene was made on a molecular structure
derived ab initio, as described below.
These are compared with the experimental nqcc's [1] in Tables 1 and 2.
Structure parameters are given in Z-matrix format in Table 3.
Rotational constants, calculated and experimental, are compared in
Table 4. |
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In Tables 1 and 2, 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. 35Cl
nqcc's in 1-Chloro-2-Methylpropene (MHz). |
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Calc. |
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Expt. [1] |
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35Cl |
Xaa |
- |
53.01 |
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52.591(1) |
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Xbb |
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21.64 |
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21.086(2) |
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Xcc |
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31.37 |
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31.505(1) |
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|Xab| |
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38.76 |
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39.037(99) |
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RMS |
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0.41 (1.2 %) |
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RSD |
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0.49 (1.1 %) |
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Xxx |
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38.12 |
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37.922(73) |
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Xyy |
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31.37 |
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31.505(2) |
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Xzz |
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69.49 |
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69.427(72) |
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ETA |
- |
0.097 |
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0.092 |
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Øz,a |
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23.04 |
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23.330(37) |
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Øa,CCl |
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23.76 |
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23.76 * |
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Øz,CCl |
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0.72 |
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0.43 * |
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* Calculated here corresponding to the structure given below. |
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Table 2. 37Cl
nqcc's in 1-Chloro-2-Methylpropene (MHz). |
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Calc. |
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Expt. [1] |
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37Cl |
Xaa |
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41.75 |
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41.429(3) |
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Xbb |
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17.03 |
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16.595(3) |
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Xcc |
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24.72 |
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24.833(4) |
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|Xab| |
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30.57 |
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30.659(31) |
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RMS |
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0.32 (1.2 %) |
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RSD |
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0.44 (1.1 %) |
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Xxx |
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30.04 |
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29.793(26) |
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Xyy |
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24.72 |
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24.833(4) |
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Xzz |
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54.77 |
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54.626(26) |
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ETA |
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0.097 |
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0.092 |
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Øz,a |
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23.06 |
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23.290(16) |
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Øa,CCl |
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23.78 |
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23.78 * |
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Øz,CCl |
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0.72 |
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0.49 * |
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* Calculated here corresponding to the structure given below. |
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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]. 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.[3]. The CH bond
lengths were corrected using r = 1.001 ropt, where ropt
is obtained by MP2/6-31G(d,p) optimization [4]. Interatomic angles
used in the calculation are those given by MP2/6-311+G(d,p) optimization. |
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Table 3. Z-Matrix (Å and degrees). |
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C |
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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 |
A8 |
3 |
180. |
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Cl |
4 |
R5 |
2 |
A9 |
3 |
0. |
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H |
1 |
R6 |
2 |
A1 |
3 |
180. |
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H |
1 |
R7 |
2 |
A2 |
3 |
- D1 |
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H |
1 |
R7 |
2 |
A2 |
3 |
D1 |
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H |
3 |
R8 |
2 |
A6 |
6 |
0. |
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H |
3 |
R9 |
2 |
A7 |
6 |
- D2 |
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H |
3 |
R9 |
2 |
A7 |
6 |
D2 |
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R1 = 1.500 |
A3 = 116.28 |
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R2 = 1.495 |
A4 = 119.03 |
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R3 = 1.334 |
A1 = 111.89 |
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R4 = 1.081 |
A2 = 110.32 |
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R5 = 1.729 |
A6 = 112.26 |
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R6 = 1.090 |
A7 = 109.93 |
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R7 = 1.092 |
A8 = 122.43 |
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R8 = 1.087 |
A9 = 124.69 |
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R9 = 1.092 |
D1 = - 59.17 |
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D2 = 121.12 |
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Table 4. Rotational Constants (MHz). 35Cl
species. |
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Calc. ropt |
Expt. [1] |
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A |
8 451.7 |
8 400.0178(5) |
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B |
2 260.7 |
2 257.7687(2) |
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C |
1 823.7 |
1 818.7071(2) |
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[1] T.Bruhn and W.Stahl, J.Mol.Spectrosc.
202,272(2000). |
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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] I.Merke, L.Poteau, G.Wlodarczak, A.Bouddou,
and J.Demaison, J.Mol.Spectrosc. 177,232(1996). |
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[4] 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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CH3ClC=CH2 |
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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CH32CCHCl.html |
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Last
Modified 26 Oct 2003 |
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