|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
GeH3CH2Cl |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Chlorine |
|
|
|
Nuclear
Quadrupole Coupling Constants |
|
|
in Chloromethylgermane
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Calculation of the chlorine nqcc's in chloromethylgermane was made on a structure
derived by MP2/aug-cc-pVTZ(G03) optimization (ropt), and on
this same structure but with empirically corrected CCl bond
length (ropt*).
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
(percentage of the average of the magnitudes of the experimental
nqcc's). RSD is the calibration residual standard deviation for
the B1LYP/TZV(3df,2p) model for calculation of the chlorine efg's/nqcc's. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 1. 35Cl
nqcc's in 74GeH3-CH2Cl (MHz). Calculation
was made on the ropt and ropt* structures. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc /ropt |
|
Calc /ropt* |
|
Expt [1]
|
|
|
|
|
|
|
|
|
|
|
|
Xaa |
- |
30.34 |
- |
30.28 |
-
|
29.7(4)
|
|
|
Xbb |
|
- 7.35
|
|
- 7.41
|
|
- 7.65**
|
|
|
Xcc |
|
37.69 |
|
37.64 |
|
37.35**
|
|
|
|Xab| |
|
54.49 |
|
54.42 |
|
|
|
|
|
|
|
|
|
|
|
|
|
RMS
|
|
0.45 (1.8 %)
|
|
0.37 (1.5 %)
|
|
|
|
|
RSD |
|
0.49 (1.1 %) |
|
0.49 (1.1 %) |
|
|
|
|
|
|
|
|
|
|
|
|
|
Xxx |
|
36.85 |
|
36.79 |
|
|
|
|
Xyy |
|
37,69 |
|
37.64 |
|
|
|
|
Xzz |
- |
74.54 |
- |
74.43 |
|
|
|
|
ETA |
|
0.0113 |
|
0.0114 |
|
|
|
|
Øz,a |
|
39.04 |
|
39.08 |
|
|
|
|
Øa,CCl |
|
39.44 |
|
39.48 |
|
|
|
|
Øz,CCl |
|
0.40 |
|
0.40 |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
** Calculated here from experimental Xaa and Xbb - Xcc = -45.0(4) MHz.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 2. 37Cl
nqcc's in 74GeH3-CH2Cl (MHz). Calculation
was made on the ropt and ropt* structures. |
|
|
|
|
|
|
|
|
|
|
|
|
|
Calc /ropt |
|
Calc /ropt* |
|
Expt [1]
|
|
|
|
|
|
|
|
|
|
|
|
Xaa |
- |
24.24 |
- |
24.15 |
-
|
23.5(6)
|
|
|
Xbb |
|
- 5.46
|
|
- 5.51
|
|
- 5.75**
|
|
|
Xcc |
|
29.71 |
|
29.66 |
|
29.25**
|
|
|
|Xab| |
|
42.88 |
|
42.82 |
|
|
|
|
|
|
|
|
|
|
|
|
|
RMS |
|
0.53 (2.7 %)
|
|
0.47 (2.4 %) |
|
|
|
|
RSD
|
|
0.44 (1.1 %)
|
|
0.44 (1.1 %)
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
** Calculated here from experimental Xaa and Xbb - Xcc = -35.0(4) MHz.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 3. GeH3CH2Cl.
MP2/aug-cc-pVTZ optimized molecular structure parameters (Å and
degrees). Corrected CCl bond lenght is given in parentheses.
|
|
|
|
|
|
Cl
C,1,B1
Ge,2,B2,1,A1
H,2,B3,1,A2,3,D1,0
H,2,B3,1,A2,3,-D1,0
H,3,B5,2,A4,1,D3,0
H,3,B5,2,A4,1,-D3,0
H,3,B7,2,A6,1,D5,0
|
|
|
|
B1=1.7898282 (1.7866)
B2=1.94884328
B3=1.08618643
B5=1.51328887
B7=1.51848712
A1=109.76947262
A2=107.30932086
A4=108.55595361
A6=108.7627165
D1=-121.59892295
D3=-60.04976111
D5=180.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table 4. 74GeH3CH235Cl. Rotational
Constants (MHz). |
|
|
|
|
|
|
|
ropt |
ropt* |
Expt [1]
|
|
|
|
|
|
|
A |
20750. |
20776. |
20655.77(46)
|
|
B |
2106.
|
2109.
|
2086.54(4)
|
|
C |
1982.
|
1985.
|
1964.04(4)
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
[1] J.Nakagawa and M.Hayashi, Bull.Chem.Soc.Jpn. 49(12),3441(1976).
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
CH3Cl |
CH3CH2Cl |
SiH3CH2Cl
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Table of Contents |
|
|
|
|
|
Molecules/Chlorine |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
GeH3CH2Cl.html |
|
|
|
|
|
|
Last
Modified 24 Aug 2015 |
|
|
|
|
|
|
|
|
|
|