Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -154.299731 |
| Energy at 298.15K | |
| HF Energy | -154.299731 |
| Nuclear repulsion energy | 74.859204 |
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 B1B95/6-31+G**
| 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' |
3871 |
3703 |
18.68 |
|
|
|
| 2 |
A' |
3187 |
3048 |
8.20 |
|
|
|
| 3 |
A' |
3026 |
2895 |
62.96 |
|
|
|
| 4 |
A' |
1525 |
1459 |
0.17 |
|
|
|
| 5 |
A' |
1484 |
1419 |
5.53 |
|
|
|
| 6 |
A' |
1422 |
1361 |
6.18 |
|
|
|
| 7 |
A' |
1222 |
1169 |
47.00 |
|
|
|
| 8 |
A' |
1066 |
1020 |
101.00 |
|
|
|
| 9 |
A' |
1006 |
962 |
43.45 |
|
|
|
| 10 |
A' |
624 |
597 |
25.07 |
|
|
|
| 11 |
A' |
380 |
364 |
36.78 |
|
|
|
| 12 |
A" |
3299 |
3156 |
9.52 |
|
|
|
| 13 |
A" |
3068 |
2934 |
47.92 |
|
|
|
| 14 |
A" |
1288 |
1232 |
0.23 |
|
|
|
| 15 |
A" |
1171 |
1120 |
0.90 |
|
|
|
| 16 |
A" |
811 |
776 |
0.09 |
|
|
|
| 17 |
A" |
250 |
239 |
142.34 |
|
|
|
| 18 |
A" |
138i |
132i |
1.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14280.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 13660.6 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.109 |
-0.370 |
0.000 |
| C2 |
0.000 |
0.535 |
0.000 |
| C3 |
1.257 |
-0.250 |
0.000 |
| H4 |
-1.922 |
0.145 |
0.000 |
| H5 |
-0.041 |
1.177 |
0.888 |
| H6 |
-0.041 |
1.177 |
-0.888 |
| H7 |
1.670 |
-0.623 |
-0.928 |
| H8 |
1.670 |
-0.623 |
0.928 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4317 | 2.3690 | 0.9622 | 2.0799 | 2.0799 | 2.9411 | 2.9411 |
C2 | 1.4317 | | 1.4812 | 1.9608 | 1.0971 | 1.0971 | 2.2339 | 2.2339 | C3 | 2.3690 | 1.4812 | | 3.2027 | 2.1233 | 2.1233 | 1.0827 | 1.0827 | H4 | 0.9622 | 1.9608 | 3.2027 | | 2.3219 | 2.3219 | 3.7884 | 3.7884 | H5 | 2.0799 | 1.0971 | 2.1233 | 2.3219 | | 1.7763 | 3.0770 | 2.4838 | H6 | 2.0799 | 1.0971 | 2.1233 | 2.3219 | 1.7763 | | 2.4838 | 3.0770 | H7 | 2.9411 | 2.2339 | 1.0827 | 3.7884 | 3.0770 | 2.4838 | | 1.8570 | H8 | 2.9411 | 2.2339 | 1.0827 | 3.7884 | 2.4838 | 3.0770 | 1.8570 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.827 |
|
O1 |
C2 |
H5 |
109.963 |
| O1 |
C2 |
H6 |
109.963 |
|
C2 |
O1 |
H4 |
108.383 |
| C2 |
C3 |
H7 |
120.422 |
|
C2 |
C3 |
H8 |
120.422 |
| C3 |
C2 |
H5 |
109.988 |
|
C3 |
C2 |
H6 |
109.988 |
| H5 |
C2 |
H6 |
108.104 |
|
H7 |
C3 |
H8 |
118.088 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.511 |
|
|
|
| 2 |
C |
-0.226 |
|
|
|
| 3 |
C |
-0.206 |
|
|
|
| 4 |
H |
0.345 |
|
|
|
| 5 |
H |
0.139 |
|
|
|
| 6 |
H |
0.139 |
|
|
|
| 7 |
H |
0.160 |
|
|
|
| 8 |
H |
0.160 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.139 |
1.688 |
0.000 |
1.694 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.023 |
-3.185 |
0.000 |
| y |
-3.185 |
-20.569 |
0.000 |
| z |
0.000 |
0.000 |
-19.077 |
|
| Traceless |
| | x | y | z |
| x |
2.801 |
-3.185 |
0.000 |
| y |
-3.185 |
-2.519 |
0.000 |
| z |
0.000 |
0.000 |
-0.281 |
|
| Polar |
| 3z2-r2 | -0.562 |
| x2-y2 | 3.547 |
| xy | -3.185 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.020 |
-0.257 |
0.000 |
| y |
-0.257 |
4.050 |
0.000 |
| z |
0.000 |
0.000 |
3.879 |
<r2> (average value of r
2) Å
2
| <r2> |
50.448 |
| (<r2>)1/2 |
7.103 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -154.301520 |
| Energy at 298.15K | -154.306051 |
| HF Energy | -154.301520 |
| Nuclear repulsion energy | 75.248449 |
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 B1B95/6-31+G**
| 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 |
3908 |
3738 |
34.41 |
|
|
|
| 2 |
A |
3318 |
3174 |
4.07 |
|
|
|
| 3 |
A |
3200 |
3061 |
4.99 |
|
|
|
| 4 |
A |
2985 |
2856 |
55.72 |
|
|
|
| 5 |
A |
2932 |
2805 |
61.27 |
|
|
|
| 6 |
A |
1496 |
1431 |
10.18 |
|
|
|
| 7 |
A |
1468 |
1404 |
5.20 |
|
|
|
| 8 |
A |
1415 |
1353 |
1.32 |
|
|
|
| 9 |
A |
1262 |
1208 |
63.46 |
|
|
|
| 10 |
A |
1223 |
1170 |
10.85 |
|
|
|
| 11 |
A |
1145 |
1095 |
64.17 |
|
|
|
| 12 |
A |
1069 |
1022 |
18.56 |
|
|
|
| 13 |
A |
959 |
917 |
12.63 |
|
|
|
| 14 |
A |
879 |
841 |
16.00 |
|
|
|
| 15 |
A |
450 |
431 |
39.19 |
|
|
|
| 16 |
A |
405 |
387 |
50.77 |
|
|
|
| 17 |
A |
267 |
255 |
103.36 |
|
|
|
| 18 |
A |
90 |
86 |
31.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14234.0 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 13616.2 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 B1B95/6-31+G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.103 |
-0.377 |
-0.058 |
| C2 |
-0.008 |
0.520 |
0.034 |
| C3 |
1.245 |
-0.253 |
-0.015 |
| H4 |
-1.914 |
0.112 |
0.106 |
| H5 |
-0.068 |
1.093 |
0.978 |
| H6 |
-0.034 |
1.258 |
-0.782 |
| H7 |
2.184 |
0.243 |
-0.222 |
| H8 |
1.240 |
-1.297 |
0.269 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4185 | 2.3520 | 0.9606 | 2.0744 | 2.0832 | 3.3492 | 2.5385 |
C2 | 1.4185 | | 1.4737 | 1.9501 | 1.1049 | 1.1002 | 2.2246 | 2.2169 | C3 | 2.3520 | 1.4737 | | 3.1823 | 2.1265 | 2.1226 | 1.0818 | 1.0817 | H4 | 0.9606 | 1.9501 | 3.1823 | | 2.2646 | 2.3741 | 4.1130 | 3.4580 | H5 | 2.0744 | 1.1049 | 2.1265 | 2.2646 | | 1.7671 | 2.6893 | 2.8149 | H6 | 2.0832 | 1.1002 | 2.1226 | 2.3741 | 1.7671 | | 2.5023 | 3.0417 | H7 | 3.3492 | 2.2246 | 1.0818 | 4.1130 | 2.6893 | 2.5023 | | 1.8715 | H8 | 2.5385 | 2.2169 | 1.0817 | 3.4580 | 2.8149 | 3.0417 | 1.8715 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.810 |
|
O1 |
C2 |
H5 |
109.966 |
| O1 |
C2 |
H6 |
110.973 |
|
C2 |
O1 |
H4 |
108.576 |
| C2 |
C3 |
H7 |
120.263 |
|
C2 |
C3 |
H8 |
119.569 |
| C3 |
C2 |
H5 |
110.292 |
|
C3 |
C2 |
H6 |
110.267 |
| H5 |
C2 |
H6 |
106.523 |
|
H7 |
C3 |
H8 |
119.782 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.529 |
|
|
|
| 2 |
C |
-0.194 |
|
|
|
| 3 |
C |
-0.240 |
|
|
|
| 4 |
H |
0.349 |
|
|
|
| 5 |
H |
0.144 |
|
|
|
| 6 |
H |
0.146 |
|
|
|
| 7 |
H |
0.151 |
|
|
|
| 8 |
H |
0.174 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.287 |
1.901 |
0.415 |
1.967 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.230 |
-2.004 |
-0.592 |
| y |
-2.004 |
-19.511 |
-0.393 |
| z |
-0.592 |
-0.393 |
-20.844 |
|
| Traceless |
| | x | y | z |
| x |
3.948 |
-2.004 |
-0.592 |
| y |
-2.004 |
-0.974 |
-0.393 |
| z |
-0.592 |
-0.393 |
-2.974 |
|
| Polar |
| 3z2-r2 | -5.948 |
| x2-y2 | 3.281 |
| xy | -2.004 |
| xz | -0.592 |
| yz | -0.393 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.824 |
-0.216 |
-0.077 |
| y |
-0.216 |
4.238 |
0.019 |
| z |
-0.077 |
0.019 |
3.740 |
<r2> (average value of r
2) Å
2
| <r2> |
50.245 |
| (<r2>)1/2 |
7.088 |