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HNSO |
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Deuterium and Nitrogen
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Nuclear
Quadrupole Coupling Constants |
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in Thionylimide |
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Deuterium and nitrogen nqcc's have been reported for thionylimide
[1-3]. A substitution structure was published by Kirchhoff in 1969
[3], and later modified with respect to the NH bond length by Dal Borgo
et al. [4]. An equilibrium structure was derived by Demaison et al. [5]. |
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Calculation of the nqcc's was made here
on the modified molecular structure of Kirchhoff, and on the equilibrium structure of Demaison et al. These nqcc's are
compared with the experimental values in Tables 1-3. The structure
parameters are shown in Table 4. |
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In Tables 1 - 3, 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 model for calculation of the nqcc's,
B3LYP/6-31G(df,3p) for deuterium and B3PW91/6-311+G(df,pd) for nitrogen. |
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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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Table 1. Deuterium nqcc's
in DNSO (kHz). Calculation was made on the re and rs structures. |
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Calc / re
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Calc / rs |
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Expt. [1] |
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Xaa |
- |
117.4 |
- |
111.8 |
- |
114.9(31) |
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Xbb |
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233.8 |
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222.9 |
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225.4 |
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Xcc |
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116.5 |
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111.0 |
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110.6 |
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|Xab| |
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14.0 |
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12.7 |
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RMS |
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6.1 (8.0 %) |
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2.3 (1.6 %) |
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RSD |
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1.1 (0.9 %) |
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1.1 (0.9 %) |
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Xxx |
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117.9 |
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112.3 |
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115.4 * |
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Xyy |
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116.5 |
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111.0 |
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110.6 |
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Xzz |
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234.4 |
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223.4 |
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225.9 |
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ETA |
- |
0.006 |
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0.006 |
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0.021 |
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Øz,a |
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92.29 |
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92.2 |
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92.1 |
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Øa,ND |
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91.00 |
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90.8 |
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90.8 |
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Øz,ND |
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1.28 |
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1.3 |
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1.3 |
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* Calculated here from the experimental
diagonal nqcc's and the calculated off-diagonal |Xab| = 12.7 kHz. |
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Table 2. 14N nqcc's
in DNSO (MHz). Calculation was made on the re and rs 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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1.294 |
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1.309 |
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1.4211(19) |
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Xbb |
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0.258 |
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0.224 |
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0.1863 |
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Xcc |
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1.552 |
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1.533 |
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1.6074 |
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|Xab| |
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2.112 |
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2.109 |
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RMS |
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0.090 (8.4 %) |
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0.080 (7.5 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Xxx |
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1.398 |
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1.411 |
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1.394 * |
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Xyy |
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1.552 |
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1.533 |
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1.6074 |
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Xzz |
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2.950 |
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2.944 |
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3.001 |
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ETA |
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0.052 |
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0.041 |
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0.071 |
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Øz,a |
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38.11 |
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37.8 |
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36.8 |
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Øa,bi |
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33.03 |
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32.9 |
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32.9 |
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Øz,bi ** |
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5.08 |
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4.8 |
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3.9 |
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* Calculated here from the experimental
diagonal nqcc's and the calculated off-diagonal |Xab| = 2.109 MHz. |
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** Angle between the z-principal axis of
the nqcc tensor and the bisector ('bi') of the DNS angle. |
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Table 3. 14N nqcc's
in HNSO (MHz). Calculation was made on the re and rs 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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1.471 |
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1.487 |
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1.5756(29) |
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Xbb |
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0.081 |
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0.046 |
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0.0254 |
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Xcc |
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1.552 |
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1.533 |
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1.6010 |
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|Xab| |
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2.060 |
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2.055 |
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RMS |
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0.074 (6.9 %) |
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0.066 (6.2 %) |
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RSD |
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0.030 (1.3 %) |
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0.030 (1.3 %) |
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Xxx |
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1.398 |
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1.411 |
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1.18(3) |
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Xyy |
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1.552 |
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1.533 |
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1.604(3) |
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Xzz |
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2.950 |
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2.944 |
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2.78(3) |
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ETA |
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0.052 |
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0.041 |
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Øz,a |
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35.68 |
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35.3 |
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33.49(8) |
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Øa,bi |
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30.60 |
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30.5 |
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Øz,bi * |
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5.08 |
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4.8 |
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3.0 |
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* Angle between the z-principal axis of
the nqcc tensor and the bisector ('bi') of the DNS angle. |
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Table 4. Molecular structure parameters, re [5] and rs [3,4] (Å
and degrees). |
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re
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rs
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HN |
1.020(1) |
1.0272 |
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NS |
1.510(2) |
1.5123 |
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SO |
1.448(1) |
1.4513 |
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HNS |
115.94(39) |
114.8 |
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NSO |
120.44(10) |
120.41 |
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[1] N.Heineking and M.C.L.Gerry, J.Mol.Spectrosc. 158,62(1993). |
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[2] P.Cassoux, A.Serafini, G.Fong, and R.L.Kuczkowski, Inorg.Chem.
17,1204(1978). |
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[3] W.H.Kirchhoff, J.Am.Chem.Soc. 91,2437(1969). |
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[4] A.DalBorgo, G.DiLonardo, F.Scappini, and A.Trombetti, Chem.
Phys.Lett. 63,115(1979). |
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[5] J.Demaison, L.Margulès, J.E.Boggs, and H.D.Rudolph, Struct.Chem. 12,1(2001). |
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HNCO |
ClNCO |
HNCSe |
HNCS |
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Table of Contents |
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Molecules/Deuterium |
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Molecules/Nitrogen |
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HNSO.html |
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Last
Modified 31 Jan 2009 |
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