|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH2ICN |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Iodine
and Nitrogen |
|
|
|
Nuclear
Quadrupole Coupling Constants |
|
|
|
in
Iodoacetonitrile |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Calculation was made of the I and N
nqcc
tensors in CH2ICN
on an ~re structure given by MP2/6-311+G(3df,3pd)
optimization with empirically corrected C-C and CN bond lengths. These
calculated nqcc's are compared with experimental values [1] in Tables 1
and 2.
Structure
parameters are given in Table 3, rotational constants in Table 4. |
|
|
|
|
|
|
|
|
|
|
|
|
In Tables 1 and 2, 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, these are perpendicular to the molecular symmetry
plane.
Ø (degrees) is the angle between its subscripted
parameters. ETA = (Xxx - Xyy)/Xzz. |
|
|
RMS is the root mean
square difference between calculated and experimental diagonal nqcc's
(percent of average of magnitudes of experimental nqcc's). RSD is
the calibration residual standard deviation for the B1LYP/6-311G(df,p)
model for calculation of the chlorine nqcc's, which may be taken as an
estimate of the uncertainty in the calculated nqcc's. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 1. Iodine nqcc's
in CH2ICN (MHz). Calculation was made on ~re
structure. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc. |
|
Expt. [1] |
|
|
|
|
|
|
|
|
|
|
127I |
Xaa |
- |
1384.1 |
- |
1276 |
|
|
|
Xbb |
|
296.4 |
|
233 |
|
|
|
Xcc |
|
1087.6 |
|
1043 |
|
|
|
|Xab| |
|
1383.6 |
|
1370 |
|
|
|
|
|
|
|
|
|
|
|
RMS |
|
76.8 (9.03 %) |
|
|
|
|
|
RSD |
|
15.2 (1.23 %) |
|
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
1074.9 |
|
1043 |
|
|
|
Xyy |
|
1087.6 |
|
1043 |
|
|
|
Xzz |
- |
2162.6 |
- |
2086 |
|
|
|
ETA |
|
0.0059 |
|
|
|
|
|
Øz,a |
|
29.36 |
|
|
|
|
|
Øa,CI |
|
30.19 |
|
|
|
|
|
Øz,CI |
|
0.83 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 2. Nitrogen nqcc's
in CH2ICN (MHz). Calculation was made on ~re
structure. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc. |
|
Expt. |
|
|
|
|
|
|
|
|
|
|
14N |
Xaa |
- |
1.911 |
|
|
|
|
|
Xbb |
- |
0.165 |
|
|
|
|
|
Xcc |
|
2.076 |
|
|
|
|
|
|Xab| |
|
3.114 |
|
|
|
|
|
|
|
|
|
|
|
|
|
RSD |
|
0.030 (1.3 %) |
|
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
2.196 |
|
|
|
|
|
Xyy |
|
2.076 |
|
|
|
|
|
Xzz |
- |
4.272 |
|
|
|
|
|
ETA |
- |
0.028 |
|
|
|
|
|
Øz,a |
|
37.17 |
|
|
|
|
|
Øa,CN |
|
37.42 |
|
|
|
|
|
Øz,CN |
|
0.24 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 3. CH2ICN.
Heavy atom structure parameters, ~re (Å and
degrees). Complete structure is given
here in Z-matrix format. |
|
|
|
|
|
CI |
2.1358 |
|
|
CC |
1.4497 |
|
|
CN |
1.1568 |
|
|
CCI |
111.58 |
|
|
CCN |
179.19 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 4. CH2ICN.
Rotational constants (MHz). |
|
|
|
|
|
|
~re |
Expt. [1] |
|
|
|
|
|
A |
20418.75 |
20037(3) |
|
B |
1751.37 |
1747.9(4) |
|
C |
1629.58 |
1622.8(4) |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
[1] R.C.Clayton, G.M.Ault, and
J.D.Graybeal, Talk TG12, 40th Ohio State University Symposium on
Mplecular Spectroscopy, 1985. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH2BrCN |
CH2ClCN |
CH2ICl |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table of Contents |
|
|
|
|
|
Molecules/Iodine |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH2ICN.html |
|
|
|
|
|
|
Last
Modified 22 Nov 2009 |
|
|
|
|
|
|
|
|
|
|