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O=C(CN)2
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Nitrogen
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Nuclear
Quadrupole Coupling Constants |
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in Carbonyl Cyanide |
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Calculation of the 14N nqcc's in O=C(CN)2 were made on the re strcuture of Demaison
et al. [1]. These are compared with the experimental values of
Lees [2] in Table 1. Structure parameters are given in Table 2.
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In Table 1, 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 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. Nitrogen nqcc's
in O=C(CN)2 (MHz). |
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Calc. |
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Expt. [2]
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14N |
Xaa |
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3.002 |
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2.846(24)
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Xbb |
- |
0.019 |
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0.045(16)
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Xcc |
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3.021 |
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2.801(32)
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Xab |
± |
2.992 |
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RMS
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0.160 (8.4 %)
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RSD
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0.030 (1.3 %)
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Xxx |
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1.832 |
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Xyy |
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3.021 |
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Xzz |
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4.853 |
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ETA |
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0.245 |
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Øz,a |
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58.25 |
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Øa,CN |
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58.14 |
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Øz,CN |
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0.11 |
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Table 2. Molecular structure parameters, re [1] (Å
and degrees). |
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OC |
1.204 |
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CC |
1.461 |
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CN |
1.159 |
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OCC |
122.63 |
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CCN |
179.23 |
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CN tilts outward. |
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[1] J.Demaison, G.Wlodarczak, H.Rück, K.H.Wiedenmann, and
H.D.Rudolph, J.Mol.Struct. 376,399(1996). |
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[2] R.M.Lees, Can.J.Phys. 49,367(1971).
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S(CN)2 |
H2C(CN)2 |
H2C=C(CN)2 |
CH3C(=O)CN
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H2C=O |
O=CCl2 |
O=CBr2 |
HC(=O)CN
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The
B3PW91/6-311+G(df,pd) model for calculation of the electric field
gradients appears to not perform well for X-C(=O)CN type molecules.
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Table of Contents |
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Molecules/Nitrogen |
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OCCNCN.html |
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Last
Modified 14 Jan 2004 |
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