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ClCH2CH2PH2 |
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Chlorine |
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Nuclear
Quadrupole Coupling Constants |
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in (2-Chloroethyl)phosphine
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(2-Chloroethyl)phosphine has been
investigated by microwave spectroscopy by Møllendal et al. [1].
The spectra of two rotameric forms, denoted I and II in the
following figure, have been observed. Hyperfine structure due to
nuclear quadrupole coupling, however, was not resolved. |
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Rotamer I Cs |
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Rotamer II C1 |
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Calculation of the chlorine nqcc
tensors
was made here on a molecular structure given by MP2/aug-cc-pVTZ(G03)
optimization, and on this same structure but with approximate equilibrium C-C and CCl bond
lengths.
The former is herein referred to as ropt, the latter
as ~re. |
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These calculated nqcc tensors are
given in Tables 1 and 2 for rotamer I, and in Tables 3 and 4 for
rotamer II. Structure parameters are given in Table 5, rotational
constants in Table 6. |
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In Tables 1 - 4,
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
subscriped axes. ETA = (Xxx - Xyy)/Xzz. |
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RSD is the calibration residual
standard deviation of
the B1LYP/TZV(3df,2p) model for calculation of the chlorine nqcc's,
which may be taken as estimate of the uncertainty inherent in the model
for calculation of the nqcc's. |
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Table 1. 35Cl
nqcc's in ClCH2CH2PH2
Rotamer I (MHz). Calculation was made on the ropt and ~re
structures. |
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35Cl
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Calc/ ropt |
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Calc/ ~re |
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Expt. |
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Xaa |
- |
57.20 |
- |
57.11 |
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Xbb |
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21.27 |
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21.24 |
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Xcc |
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35.92 |
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35.87 |
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|Xab| |
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35.22 |
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35.18 |
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RSD |
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0.49 (1.1 %) |
0.49 (1.1 %) |
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Xxx |
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34.76 |
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34.71 |
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Xyy |
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35.92 |
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35.87 |
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Xzz |
- |
70.69 |
- |
70.59 |
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ETA |
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0.016 |
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0.016 |
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Øz,a |
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20.96 |
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20.96 |
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Øa,CCl |
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20.31 |
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20.31 |
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Øz,CCl |
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0.65 |
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0.65 |
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Table 2. 37Cl
nqcc's in ClCH2CH2PH2
Rotamer I (MHz). Calculation was made on the ropt and ~re
structures. |
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Calc/ ropt |
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Calc/ ~re |
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Expt. |
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Xaa |
- |
45.12 |
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45.05 |
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Xbb |
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16.80 |
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16.78 |
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Xcc |
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28.31 |
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28.27 |
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|Xab| |
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27.72 |
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27.68 |
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RSD |
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0.49 (1.1 %) |
0.49 (1.1 %) |
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Xxx |
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27.40 |
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27.36 |
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Xyy |
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28.31 |
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28.27 |
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Xzz |
- |
55.71 |
- |
55.63 |
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ETA |
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0.016 |
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0.016 |
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Øz,a |
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20.92 |
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20.92 |
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Øa,CCl |
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20.27 |
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20.27 |
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Øz,CCl |
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0.65 |
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0.65 |
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Table 3. 35Cl
nqcc's in ClCH2CH2PH2
Rotamer II (MHz). Calculation was made on the ropt and ~re
structures. |
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Calc/ ropt |
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Calc/ ~re |
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Expt. |
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Xaa |
- |
58.41 |
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58.31 |
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Xbb |
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22.06 |
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22.02 |
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Xcc |
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36.35 |
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36.29 |
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Xab |
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35.37 |
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35.32 |
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Xac |
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0.39 |
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0.39 |
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Xbc |
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- 0.18 |
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- 0.18 |
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RSD |
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0.49 (1.1 %) |
0.49 (1.1 %) |
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Xxx |
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35.40 |
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35.34 |
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Xyy |
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36.35 |
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36.29 |
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Xzz |
- |
71.75 |
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71.64 |
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ETA |
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0.013 |
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0.013 |
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Øz,CCl |
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0.75 |
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0.76 |
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Table 4. 37Cl
nqcc's in ClCH2CH2PH2
Rotamer II (MHz). Calculation was made on the ropt and ~re
structures. |
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Calc/ ropt |
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Calc/ ~re |
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Expt. |
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Xaa |
- |
46.07 |
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46.00 |
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Xbb |
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17.42 |
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17.39 |
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Xcc |
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28.65 |
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28.60 |
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Xab |
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27.83 |
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27.80 |
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Xac |
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0.30 |
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0.30 |
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Xbc |
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- 0.14 |
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- 0.14 |
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RSD |
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0.49 (1.1 %) |
0.49 (1.1 %) |
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Xxx |
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27.90 |
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27.85 |
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Xyy |
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28.65 |
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28.60 |
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Xzz |
- |
56.55 |
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56.46 |
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ETA |
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0.013 |
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0.013 |
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Øz,CCl |
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0.75 |
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0.76 |
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Table 5. (2-Chloroethyl)phosphine.
Heavy atom structure parameters, ropt and ~ re
(Å and degrees). Complete structures are given here in Z-matrix format. |
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Rotamer
I |
Rotamer
II |
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ropt |
~ re |
ropt |
~ re |
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ClC |
1.7966 |
1.7933 |
1.7907 |
1.7875 |
CC |
1.5098 |
1.5082 |
1.5132 |
1.5115 |
CP |
1.8620 |
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1.8694 |
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ClCC |
111.13 |
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110.95 |
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CCP |
113.74 |
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111.71 |
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ClCCP |
180. |
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177.75 |
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Table 6. 35ClCH2CH2PH2
Rotational Constants (MHz), ropt and
~ re. |
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Rotamer
I |
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ropt |
~ re |
Expt [1] |
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A |
24440.22 |
24465.65 |
24287(16) |
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B |
1451.93 |
1454.59 |
1445.8842(23) |
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C |
1410.88 |
1413.48 |
1404.8867(25) |
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Rotamer
II |
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ropt |
~ re |
Expt [1] |
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A |
24648.62 |
24675.71 |
24547(17) |
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B |
1461.71 |
1464.44 |
1456.0328(43) |
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C |
1418.43 |
1421.08 |
1412.9167(54) |
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[1] H.Møllendal, A.Konovalov,
and J.-C.Guillemin, J.Phys.Chem. A, 113, 12904(2009). |
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Calculation
of Cl and N Nuclear Quadrupole Coupling Constants on Approximate
Equilibrium Molecular Structures: F, Cl, CN - Ethanes. |
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Table of Contents |
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Molecules/Chlorine |
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ClCH2CH2PH2.html |
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Last
Modified 16 Nov 2009 |
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