|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH2(CN)2 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Nitrogen and Deuterium |
|
|
|
Nuclear
Quadrupole Coupling Constants |
|
|
|
in Dicyanomethane |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Dicyanomethane has been the subject of a number of microwave
investigations [1-8]. Randell et al. [6] measured the nitrogen nqcc's
in the mixed species, and determined the ground state average structure.
Cox et al. [7] measured the nqcc's in the normal species. An equilibrium
structure was determined by Demaison et al. [8]. |
|
|
|
|
|
|
|
|
|
|
|
|
Calculation was made here of the
nitrogen and deuterium nqcc's on both the average and equilibrium
molecular structures. These nitrogen nqcc's are compared with the
experimental nqcc's in the mixed species in Table 1, and in the normal
species in Table 2. Calculated deuterium nqcc's are shown in
Table 3. In Table 4, the structures are compared. |
|
|
|
|
|
|
|
|
|
|
|
|
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 B3PW91/6-311+G(df,pd) model
for calculation of the nitrogen nqcc's. |
|
|
|
|
|
|
|
|
|
|
|
|
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. Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 1. Nitrogen
nqcc's in CH2(C14N)(C15N) (MHz). Calculation was made on
the rz and re structures. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc. rz
|
|
Calc. re |
|
Expt. [6] |
|
|
|
|
|
|
|
|
|
|
|
Xaa |
- |
2.365 |
- |
2.352 |
- |
2.364(9) |
|
|
Xbb |
|
0.340 |
|
0.291 |
|
0.313(6) |
|
|
Xcc |
|
2.024 |
|
2.061 |
|
2.051(6) |
|
|
|Xab| |
|
3.019 |
|
3.074 |
|
|
|
|
|
|
|
|
|
|
|
|
|
RMS |
|
0.022 (1.4 %) |
0.016 (1.0 %) |
|
|
|
RSD |
|
0.030 (1.3 %) |
0.030 (1.3 %) |
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
|
|
2.315 |
|
2.327 * |
|
|
Xyy |
|
|
|
2.061 |
|
2.051(6) |
|
|
Xzz |
|
|
- |
4.376 |
- |
4.378 |
|
|
ETA |
|
|
- |
0.058 |
- |
0.063 |
|
|
Øz,a |
|
|
|
33.37 |
|
33.23 |
|
|
Øa,CN |
|
|
|
33.34 |
|
33.34 |
|
|
Øz,CN |
|
|
|
0.03 |
|
0.11 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
* Calculated here from the experimental diagonal
nqcc's and the calculated off-diagonal nqcc. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 2. Nitrogen
nqcc's in CH2(CN)2 (MHz). Calculation was made on
the rz and re structures. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc. rz
|
|
Calc. re |
|
Expt. [7] |
|
|
|
|
|
|
|
|
|
|
|
Xaa |
- |
2.412 |
- |
2.400 |
- |
2.368(28) |
|
|
Xbb |
|
0.387 |
|
0.339 |
|
0.318(20) |
|
|
Xcc |
|
2.024 |
|
2.061 |
|
2.050(20) |
|
|
|Xab| |
± |
2.998 |
± |
3.052 |
|
|
|
|
|
|
|
|
|
|
|
|
|
RMS |
|
0.050 (3.1 %) |
0.023 (1.4 %) |
|
|
|
RSD |
|
0.030 (1.3 %) |
0.030 (1.3 %) |
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
|
|
2.315 |
|
2.309 * |
|
|
Xyy |
|
|
|
2.061 |
|
2.050(20) |
|
|
Xzz |
|
|
- |
4.376 |
- |
4.359 |
|
|
ETA |
|
|
- |
0.058 |
- |
0.059 |
|
|
Øz,a |
|
|
|
32.92 |
|
33.12 |
|
|
Øa,CN |
|
|
|
32.89 |
|
32.89 |
|
|
Øz,CN |
|
|
|
0.03 |
|
0.23 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
* Calculated here from the experimental diagonal
nqcc's and the calculated off-diagonal nqcc. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 3. Deuterium
nqcc's in CD2(CN)2 (kHz). Calculation was made on
the equilibrium structure. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc. |
|
Expt. |
|
|
|
|
|
|
|
|
|
|
2H |
Xaa |
|
- 85.4 |
|
|
|
|
|
Xbb |
|
2.6 |
|
|
|
|
|
Xcc |
|
82.8 |
|
|
|
|
|
Xbc |
± |
129.9 |
|
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
- 93.2 |
|
|
|
|
|
Xyy |
|
- 85.4 |
|
|
|
|
|
Xzz |
|
178.6 |
|
|
|
|
|
ETA |
- |
0.044 |
|
|
|
|
|
Øz,b |
|
53.58 |
|
|
|
|
|
Øb,CH |
|
53.91 |
|
|
|
|
|
Øz,CH |
|
0.33 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 4. Molecular structure parameters (Å and degrees). |
|
|
|
|
|
|
|
|
rz [6] |
re [8] |
|
|
|
|
|
|
|
CC |
1.4593 |
1.464 |
|
|
CN |
1.1602 |
1.155 |
|
|
CH |
1.1090 |
1.091 |
|
|
CCC |
112.50 |
111.98 |
|
|
HCH |
106.94 |
107.82 |
|
|
CCN |
178.60 |
178.88 |
|
|
|
|
|
|
|
CN tilts outward. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
[1] N.Muller and D.E.Pritchard, J.Am.Chem.Soc. 80,3483(1958). |
|
|
[2] E.Hirota and Y.Morino, Bull.Chem.Soc.Jpn. 33,158(1960);
33,705(1960). |
|
|
[3] E.Hirota, J.Mol.Spectrosc. 7,242(1961). |
|
|
[4] R.L.Cook, R.T.Walden, and G.E.Jones, J.Mol.Spectrosc. 53,370(1974). |
|
|
[5] J.Burie, D.Boucher, J.Demaison, and A.Dubrille, J.Phys.
(Paris) 43,1319(1982). |
|
|
[6] J.Randell, A.P.Cox, I.Merke, and H.Dreizler, Chem.Soc. Faraday
Trans. 86,1981(1990). Table 6. |
|
|
[7] A.P.Cox, Y.Kawashima, E.Fliege, and H.Dreizler, Z.Naturforsch.
40a,361(1985). |
|
|
[8] J.Demaison, G.Wlodarczak, H.Rück, K.H.Wiedenmann, and
H.D.Rudolph, J.Mol.Struct. 376,399(1996). |
|
|
|
|
|
|
|
|
|
|
|
|
"Rotational
spectroscopy of malononitrile and its corresponding monoisocyanide
isomer, isocyanoacetonitrile" R.A.Motiyenko, I.A.Armieieva, L.Margulès,
E.A.Alekseev, and J.-C.Guillemin, A&A, 623,A162(2019).
Malononitile: X aa = -2.377(15) MHz and Xbb - Xcc = -1.731(17) MHz.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH3CN |
O=C(CN)2 |
H2C=C(CN)2 |
S(CN)2 |
|
|
CD2F2 |
CD2Cl2 |
CD2Br2 |
CH3D |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table of Contents |
|
|
|
|
|
Molecules/Nitrogen |
|
|
|
|
|
Molecules/Deuterium |
|
|
|
|
|
Summary/Methyls
Deuterium nqcc's in the substituted methanes. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH2CN2.html |
|
|
|
|
|
|
Last
Modified 11 May 2019 |
|
|
|
|
|
|
|
|
|
|