Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -190.630040 |
| Energy at 298.15K | |
| HF Energy | -190.630040 |
| Nuclear repulsion energy | 88.797387 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3095 |
2971 |
30.15 |
209.19 |
0.13 |
0.23 |
| 2 |
A1 |
2365 |
2271 |
963.53 |
32.61 |
0.38 |
0.55 |
| 3 |
A1 |
1827 |
1754 |
30.32 |
0.40 |
0.75 |
0.86 |
| 4 |
A1 |
1478 |
1419 |
2.47 |
15.48 |
0.56 |
0.72 |
| 5 |
A1 |
940 |
903 |
6.36 |
40.39 |
0.26 |
0.42 |
| 6 |
B1 |
1024 |
983 |
23.32 |
0.49 |
0.75 |
0.86 |
| 7 |
B1 |
665 |
638 |
27.68 |
1.29 |
0.75 |
0.86 |
| 8 |
B1 |
222 |
213 |
0.70 |
3.70 |
0.75 |
0.86 |
| 9 |
B2 |
3167 |
3040 |
10.87 |
136.80 |
0.75 |
0.86 |
| 10 |
B2 |
1064 |
1021 |
1.65 |
0.16 |
0.75 |
0.86 |
| 11 |
B2 |
482 |
463 |
16.26 |
2.29 |
0.75 |
0.86 |
| 12 |
B2 |
104i |
100i |
18.55 |
0.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8111.1 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 7787.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.865 |
| C2 |
0.000 |
0.000 |
-0.554 |
| C3 |
0.000 |
0.000 |
0.718 |
| O4 |
0.000 |
0.000 |
1.886 |
| H5 |
0.000 |
0.923 |
-2.442 |
| H6 |
0.000 |
-0.923 |
-2.442 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3111 | 2.5828 | 3.7510 | 1.0882 | 1.0882 |
C2 | 1.3111 | | 1.2717 | 2.4399 | 2.1015 | 2.1015 | C3 | 2.5828 | 1.2717 | | 1.1682 | 3.2918 | 3.2918 | O4 | 3.7510 | 2.4399 | 1.1682 | | 4.4253 | 4.4253 | H5 | 1.0882 | 2.1015 | 3.2918 | 4.4253 | | 1.8453 | H6 | 1.0882 | 2.1015 | 3.2918 | 4.4253 | 1.8453 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
122.019 |
| C2 |
C1 |
H6 |
122.019 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
115.961 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.150 |
|
|
|
| 2 |
C |
-0.113 |
|
|
|
| 3 |
C |
0.185 |
|
|
|
| 4 |
O |
-0.230 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
| 6 |
H |
0.154 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.671 |
2.671 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.467 |
0.000 |
0.000 |
| y |
0.000 |
-22.267 |
0.000 |
| z |
0.000 |
0.000 |
-21.413 |
|
| Traceless |
| | x | y | z |
| x |
-0.627 |
0.000 |
0.000 |
| y |
0.000 |
-0.327 |
0.000 |
| z |
0.000 |
0.000 |
0.954 |
|
| Polar |
| 3z2-r2 | 1.908 |
| x2-y2 | -0.200 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.242 |
0.000 |
0.000 |
| y |
0.000 |
2.909 |
0.000 |
| z |
0.000 |
0.000 |
10.264 |
<r2> (average value of r
2) Å
2
| <r2> |
81.659 |
| (<r2>)1/2 |
9.037 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -190.630431 |
| Energy at 298.15K | |
| HF Energy | -190.630431 |
| Nuclear repulsion energy | 88.956472 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3178 |
3051 |
10.45 |
127.67 |
0.70 |
0.83 |
| 2 |
A' |
3100 |
2976 |
29.37 |
176.30 |
0.13 |
0.24 |
| 3 |
A' |
2304 |
2212 |
978.28 |
36.28 |
0.40 |
0.57 |
| 4 |
A' |
1808 |
1736 |
13.67 |
1.39 |
0.50 |
0.66 |
| 5 |
A' |
1482 |
1423 |
1.12 |
15.87 |
0.58 |
0.73 |
| 6 |
A' |
1067 |
1025 |
11.60 |
4.17 |
0.11 |
0.19 |
| 7 |
A' |
956 |
918 |
4.22 |
35.04 |
0.22 |
0.36 |
| 8 |
A' |
507 |
487 |
15.94 |
4.55 |
0.58 |
0.74 |
| 9 |
A' |
125 |
120 |
21.63 |
5.54 |
0.72 |
0.84 |
| 10 |
A" |
1028 |
987 |
23.63 |
0.64 |
0.75 |
0.86 |
| 11 |
A" |
701 |
673 |
21.78 |
1.94 |
0.75 |
0.86 |
| 12 |
A" |
259 |
249 |
0.60 |
4.57 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8257.5 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 7928.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.842 |
-1.627 |
0.000 |
| C2 |
0.000 |
-0.615 |
0.000 |
| C3 |
-0.291 |
0.638 |
0.000 |
| O4 |
-0.715 |
1.722 |
0.000 |
| H5 |
1.922 |
-1.492 |
0.000 |
| H6 |
0.492 |
-2.656 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3165 | 2.5328 | 3.6934 | 1.0885 | 1.0867 |
C2 | 1.3165 | | 1.2863 | 2.4440 | 2.1124 | 2.0999 | C3 | 2.5328 | 1.2863 | | 1.1640 | 3.0714 | 3.3862 | O4 | 3.6934 | 2.4440 | 1.1640 | | 4.1570 | 4.5419 | H5 | 1.0885 | 2.1124 | 3.0714 | 4.1570 | | 1.8436 | H6 | 1.0867 | 2.0999 | 3.3862 | 4.5419 | 1.8436 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
153.344 |
|
C2 |
C1 |
H5 |
122.594 |
| C2 |
C1 |
H6 |
121.511 |
|
C2 |
C3 |
O4 |
171.749 |
| H5 |
C1 |
H6 |
115.895 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.178 |
|
|
|
| 2 |
C |
-0.188 |
|
|
|
| 3 |
C |
0.289 |
|
|
|
| 4 |
O |
-0.225 |
|
|
|
| 5 |
H |
0.149 |
|
|
|
| 6 |
H |
0.152 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.615 |
-1.897 |
0.000 |
2.491 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.817 |
-0.874 |
0.000 |
| y |
-0.874 |
-22.181 |
0.000 |
| z |
0.000 |
0.000 |
-22.539 |
|
| Traceless |
| | x | y | z |
| x |
0.543 |
-0.874 |
0.000 |
| y |
-0.874 |
-0.003 |
0.000 |
| z |
0.000 |
0.000 |
-0.540 |
|
| Polar |
| 3z2-r2 | -1.081 |
| x2-y2 | 0.364 |
| xy | -0.874 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.403 |
-2.513 |
0.000 |
| y |
-2.513 |
8.852 |
0.000 |
| z |
0.000 |
0.000 |
2.283 |
<r2> (average value of r
2) Å
2
| <r2> |
80.243 |
| (<r2>)1/2 |
8.958 |