Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -154.398522 |
| Energy at 298.15K | |
| HF Energy | -154.398522 |
| Nuclear repulsion energy | 74.596098 |
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 B3LYP/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' |
3754 |
3628 |
1.61 |
|
|
|
| 2 |
A' |
3141 |
3035 |
12.99 |
|
|
|
| 3 |
A' |
2976 |
2876 |
75.45 |
|
|
|
| 4 |
A' |
1535 |
1483 |
0.37 |
|
|
|
| 5 |
A' |
1489 |
1439 |
5.44 |
|
|
|
| 6 |
A' |
1445 |
1397 |
3.55 |
|
|
|
| 7 |
A' |
1246 |
1204 |
65.41 |
|
|
|
| 8 |
A' |
1044 |
1009 |
60.45 |
|
|
|
| 9 |
A' |
976 |
943 |
62.46 |
|
|
|
| 10 |
A' |
626 |
605 |
20.27 |
|
|
|
| 11 |
A' |
374 |
362 |
34.77 |
|
|
|
| 12 |
A" |
3244 |
3135 |
19.43 |
|
|
|
| 13 |
A" |
3004 |
2902 |
70.43 |
|
|
|
| 14 |
A" |
1296 |
1252 |
0.27 |
|
|
|
| 15 |
A" |
1174 |
1135 |
1.00 |
|
|
|
| 16 |
A" |
816 |
789 |
0.31 |
|
|
|
| 17 |
A" |
260 |
251 |
141.34 |
|
|
|
| 18 |
A" |
151i |
146i |
1.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14124.4 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 13648.4 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.113 |
-0.377 |
0.000 |
| C2 |
0.000 |
0.538 |
0.000 |
| C3 |
1.263 |
-0.244 |
0.000 |
| H4 |
-1.922 |
0.149 |
0.000 |
| H5 |
-0.042 |
1.184 |
0.888 |
| H6 |
-0.042 |
1.184 |
-0.888 |
| H7 |
1.667 |
-0.633 |
-0.927 |
| H8 |
1.667 |
-0.633 |
0.927 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4406 | 2.3799 | 0.9652 | 2.0910 | 2.0910 | 2.9414 | 2.9414 |
C2 | 1.4406 | | 1.4852 | 1.9613 | 1.0994 | 1.0994 | 2.2377 | 2.2377 | C3 | 2.3799 | 1.4852 | | 3.2097 | 2.1286 | 2.1286 | 1.0835 | 1.0835 | H4 | 0.9652 | 1.9613 | 3.2097 | | 2.3228 | 2.3228 | 3.7884 | 3.7884 | H5 | 2.0910 | 1.0994 | 2.1286 | 2.3228 | | 1.7766 | 3.0850 | 2.4944 | H6 | 2.0910 | 1.0994 | 2.1286 | 2.3228 | 1.7766 | | 2.4944 | 3.0850 | H7 | 2.9414 | 2.2377 | 1.0835 | 3.7884 | 3.0850 | 2.4944 | | 1.8545 | H8 | 2.9414 | 2.2377 | 1.0835 | 3.7884 | 2.4944 | 3.0850 | 1.8545 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.853 |
|
O1 |
C2 |
H5 |
110.095 |
| O1 |
C2 |
H6 |
110.095 |
|
C2 |
O1 |
H4 |
107.576 |
| C2 |
C3 |
H7 |
120.371 |
|
C2 |
C3 |
H8 |
120.371 |
| C3 |
C2 |
H5 |
109.993 |
|
C3 |
C2 |
H6 |
109.993 |
| H5 |
C2 |
H6 |
107.805 |
|
H7 |
C3 |
H8 |
117.692 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.563 |
|
|
|
| 2 |
C |
-0.201 |
|
|
|
| 3 |
C |
-0.403 |
|
|
|
| 4 |
H |
0.374 |
|
|
|
| 5 |
H |
0.183 |
|
|
|
| 6 |
H |
0.183 |
|
|
|
| 7 |
H |
0.213 |
|
|
|
| 8 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.230 |
1.595 |
0.000 |
1.612 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.822 |
-2.910 |
0.000 |
| y |
-2.910 |
-20.338 |
0.000 |
| z |
0.000 |
0.000 |
-18.918 |
|
| Traceless |
| | x | y | z |
| x |
2.807 |
-2.910 |
0.000 |
| y |
-2.910 |
-2.468 |
0.000 |
| z |
0.000 |
0.000 |
-0.338 |
|
| Polar |
| 3z2-r2 | -0.677 |
| x2-y2 | 3.516 |
| xy | -2.910 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.661 |
-0.478 |
0.000 |
| y |
-0.478 |
3.510 |
0.000 |
| z |
0.000 |
0.000 |
3.550 |
<r2> (average value of r
2) Å
2
| <r2> |
50.565 |
| (<r2>)1/2 |
7.111 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -154.400171 |
| Energy at 298.15K | -154.404842 |
| HF Energy | -154.400171 |
| Nuclear repulsion energy | 74.943975 |
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 B3LYP/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 |
3792 |
3664 |
7.61 |
|
|
|
| 2 |
A |
3263 |
3153 |
11.26 |
|
|
|
| 3 |
A |
3153 |
3046 |
7.96 |
|
|
|
| 4 |
A |
2942 |
2843 |
76.42 |
|
|
|
| 5 |
A |
2873 |
2776 |
81.06 |
|
|
|
| 6 |
A |
1512 |
1461 |
5.60 |
|
|
|
| 7 |
A |
1475 |
1425 |
5.40 |
|
|
|
| 8 |
A |
1432 |
1384 |
0.45 |
|
|
|
| 9 |
A |
1286 |
1243 |
72.22 |
|
|
|
| 10 |
A |
1229 |
1188 |
10.12 |
|
|
|
| 11 |
A |
1113 |
1075 |
34.11 |
|
|
|
| 12 |
A |
1074 |
1037 |
43.35 |
|
|
|
| 13 |
A |
964 |
931 |
11.99 |
|
|
|
| 14 |
A |
865 |
836 |
17.92 |
|
|
|
| 15 |
A |
459 |
443 |
29.84 |
|
|
|
| 16 |
A |
404 |
390 |
43.07 |
|
|
|
| 17 |
A |
295 |
285 |
114.48 |
|
|
|
| 18 |
A |
148 |
143 |
21.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14138.6 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 13662.1 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 B3LYP/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.110 |
-0.379 |
-0.058 |
| C2 |
-0.008 |
0.522 |
0.035 |
| C3 |
1.250 |
-0.255 |
-0.017 |
| H4 |
-1.917 |
0.119 |
0.107 |
| H5 |
-0.064 |
1.099 |
0.979 |
| H6 |
-0.030 |
1.265 |
-0.780 |
| H7 |
2.192 |
0.240 |
-0.222 |
| H8 |
1.247 |
-1.296 |
0.277 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4258 | 2.3635 | 0.9630 | 2.0857 | 2.0945 | 3.3627 | 2.5508 |
C2 | 1.4258 | | 1.4795 | 1.9526 | 1.1077 | 1.1029 | 2.2325 | 2.2218 | C3 | 2.3635 | 1.4795 | | 3.1920 | 2.1333 | 2.1283 | 1.0827 | 1.0820 | H4 | 0.9630 | 1.9526 | 3.1920 | | 2.2703 | 2.3790 | 4.1239 | 3.4703 | H5 | 2.0857 | 1.1077 | 2.1333 | 2.2703 | | 1.7670 | 2.6958 | 2.8184 | H6 | 2.0945 | 1.1029 | 2.1283 | 2.3790 | 1.7670 | | 2.5098 | 3.0502 | H7 | 3.3627 | 2.2325 | 1.0827 | 4.1239 | 2.6958 | 2.5098 | | 1.8705 | H8 | 2.5508 | 2.2218 | 1.0820 | 3.4703 | 2.8184 | 3.0502 | 1.8705 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
108.874 |
|
O1 |
C2 |
H5 |
110.197 |
| O1 |
C2 |
H6 |
111.206 |
|
C2 |
O1 |
H4 |
108.088 |
| C2 |
C3 |
H7 |
120.440 |
|
C2 |
C3 |
H8 |
119.516 |
| C3 |
C2 |
H5 |
110.263 |
|
C3 |
C2 |
H6 |
110.154 |
| H5 |
C2 |
H6 |
106.130 |
|
H7 |
C3 |
H8 |
119.561 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.568 |
|
|
|
| 2 |
C |
-0.181 |
|
|
|
| 3 |
C |
-0.433 |
|
|
|
| 4 |
H |
0.380 |
|
|
|
| 5 |
H |
0.186 |
|
|
|
| 6 |
H |
0.190 |
|
|
|
| 7 |
H |
0.205 |
|
|
|
| 8 |
H |
0.222 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.337 |
1.781 |
0.503 |
1.881 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.024 |
-1.867 |
-0.707 |
| y |
-1.867 |
-19.479 |
-0.495 |
| z |
-0.707 |
-0.495 |
-20.444 |
|
| Traceless |
| | x | y | z |
| x |
3.937 |
-1.867 |
-0.707 |
| y |
-1.867 |
-1.244 |
-0.495 |
| z |
-0.707 |
-0.495 |
-2.693 |
|
| Polar |
| 3z2-r2 | -5.386 |
| x2-y2 | 3.454 |
| xy | -1.867 |
| xz | -0.707 |
| yz | -0.495 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.689 |
-0.268 |
-0.170 |
| y |
-0.268 |
3.968 |
-0.091 |
| z |
-0.170 |
-0.091 |
3.021 |
<r2> (average value of r
2) Å
2
| <r2> |
50.425 |
| (<r2>)1/2 |
7.101 |