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CH3CH2CN
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Nitrogen
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Nuclear
Quadrupole Coupling Constants |
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in
Ethyl Cyanide |
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Calculation
of the nitrogen nqcc's in ethyl cyanide was made here on the
substitution structure of Heise et al. [1], and on an approximate
equilibrium ~re structure given by MP2/aug-cc-pVTZ
optimization with empirically corrected bond lengths.
These are
compared with the experimental nqcc's [1-4] in Tables 1-8.
Molecular structure parameters are given in Table 9. |
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Calculation was made also on each of
several molecular structures reported by Demaison et al. [5]. See PDF. |
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In Tables 1 - 8, subscripts a,b,c
refer to the
principal axes of the inertia tensor, subscripts 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 symmetry plane
of the molecule. 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 nqcc's (percentage of
average experimental nqcc). RSD is the residual standard
deviation
of calibration of the B3PW91/6-311+G(df,pd) model for calculation of
the nqcc's. |
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Table 1. 14N nqcc's in CH3CH2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [2] |
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Xaa |
- |
3.349 |
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3.322 |
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3.3572(18) |
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Xbb |
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1.278 |
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1.278 |
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1.2982(39) |
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Xcc |
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2.070 |
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2.044 |
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2.0590(39) |
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|Xab| |
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2.180 |
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2.165 |
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RMS |
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0.014 (0.63 %) |
0.025 (1.1 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Xxx |
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2.144 |
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2.136 |
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Xyy |
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2.070 |
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2.044 |
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Xzz |
- |
4.214 |
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4.181 |
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ETA |
- |
0.017 |
- |
0.022 |
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Øz,a |
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21.65 |
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21.63 |
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Øa,CN |
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21.92 |
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21.99 |
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Øz,CN |
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0.27 |
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0.36 |
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Table 2. 14N nqcc's in CH3CH2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [3] |
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Xaa |
- |
3.349 |
- |
3.322 |
- |
3.309(33) |
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Xbb |
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1.278 |
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1.278 |
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1.265(13) |
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Xcc |
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2.070 |
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2.044 |
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2.044(20) |
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|Xab| |
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2.180 |
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2.165 |
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RMS |
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0.028 (1.3 %) |
0.011 (0.48 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Xxx |
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2.144 |
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2.136 |
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Xyy |
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2.070 |
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2.044 |
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Xzz |
- |
4.214 |
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4.181 |
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ETA |
- |
0.017 |
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0.022 |
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Øz,a |
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21.65 |
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21.63 |
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Øa,CN |
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21.92 |
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21.99 |
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Øz,CN |
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0.27 |
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0.36 |
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Table 3. 14N nqcc's in CH3CD2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [1] |
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Xaa |
- |
3.441 |
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3.412 |
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3.449(16) |
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Xbb |
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1.370 |
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1.368 |
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1.399(15) |
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Xcc |
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2.070 |
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2.044 |
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2.050(17) |
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|Xab| |
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2.078 |
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2.064 |
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2.01(18) |
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RMS |
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0.021 (0.90 %) |
0.028 (1.2 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 4. 14N nqcc's in CD3CH2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [1] |
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Xaa |
- |
3.193 |
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3.166 |
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3.209(17) |
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Xbb |
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1.123 |
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1.122 |
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1.150(16) |
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Xcc |
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2.070 |
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2.044 |
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2.059(18) |
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|Xab| |
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2.334 |
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2.319 |
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2.27(12) |
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RMS |
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0.019 (0.89 %) |
0.031 (1.4 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 5. 14N nqcc's in 13CH3CH2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [1] |
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Xaa |
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3.311 |
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3.285 |
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3.290(11) |
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Xbb |
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1.241 |
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1.241 |
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1.242(10) |
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Xcc |
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2.070 |
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2.044 |
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2.048(12) |
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|Xab| |
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2.220 |
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2.204 |
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RMS |
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0.018 (0.81 %) |
0.004 (0.17 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 6. 14N nqcc's in CH313CH2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [1] |
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Xaa |
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3.368 |
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3.341 |
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3.377(21) |
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Xbb |
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1.298 |
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1.297 |
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1.334(17) |
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Xcc |
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2.070 |
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2.044 |
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2.043(19) |
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|Xab| |
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2.159 |
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2.144 |
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RMS |
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0.026 (1.2 %) |
0.030 (1.3 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 7. 14N nqcc's in CH3CH213CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [1] |
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Xaa |
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3.344 |
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3.317 |
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3.349(11) |
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Xbb |
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1.273 |
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1.273 |
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1.297(10) |
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Xcc |
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2.070 |
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2.044 |
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2.052(12) |
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|Xab| |
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2.186 |
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2.170 |
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RMS |
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0.018 (0.83 %) |
0.024 (1.0 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 8. 14N nqcc's in CD3CD2CN
(MHz). Calculation was made on the ~re and rs
[1] structures. |
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Calc / ~re |
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Calc / rs |
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Expt. [4] |
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Xaa |
- |
3.270 |
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3.241 |
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3.213(20) |
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Xbb |
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1.200 |
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1.197 |
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1.168(20) |
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Xcc |
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2.070 |
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2.044 |
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2.045(20) |
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|Xab| |
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2.261 |
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2.248 |
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RMS |
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0.040 (1.9 %) |
0.023 (1.1 %) |
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RSD |
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0.030 (1.3 %) |
0.030 (1.3 %) |
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Table 8. Molecular
structure parameters, ~re and rs [1]
(Å
and degrees). Hs lies in symmetry plane.
Complete structures are given here in Z-matrix format (Gaussian
input file). |
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~re |
rs [1] |
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NC(3) |
1.1560 |
1.159(1) |
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C(3)C(2) |
1.4611 |
1.459(1) |
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C(2)C(1) |
1.5272 |
1.537(1) |
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C(2)H |
1.0899 |
1.094(1) |
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C(1)Hs |
1.0881 |
1.079(18) |
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C(1)Ha |
1.0878 |
1.091(1) |
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NC(3)C(2) |
178.68 |
178.73(22) |
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C(3)C(2)C(1) |
111.64 |
111.98(10) |
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C(1)C(2)H |
110.73 |
110.62(3) |
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C(2)C(1)Hs |
109.88 |
111.08(237) |
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C(2)C(1)Ha |
110.67 |
110.47(2) |
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[1] H.M.Heise, H.Lutz, and
H.Dreizler, Z.Naturforsch. 29a,1345 (1974); H.Mäder, H.M.Heise,
and H.Dreizler, Z.Naturforsch. 29a,164 (1973). |
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[2] A.Kraśnicki and Z.Kisiel, J.Mol.Spectrosc. 270,83(2011).
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[3] Y.S.Li and M.D.Harmony,
J.Chem.Phys. 50,3674(1969). |
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[4] Y.S.Li
and J.R.Durig, J.Mol.Spectrosc. 54,296(1975). |
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[5] J.Demaison, L.Margulès,
H.Mäder, M.Sheng, and H.D.Rudolph, J.Mol.Spectrosc. 252,169(2008). |
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CH3CH2NC |
CH3CH2Cl |
CH3CH2Br |
CH3CN |
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Table of Contents |
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Molecules/Nitrogen |
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CH3CH2CN.html |
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Last
Modified 12 Sept 2011 |
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