Jump to
S1C2
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -114.425145 |
| Energy at 298.15K | -114.426559 |
| HF Energy | -114.425145 |
| Nuclear repulsion energy | 30.666859 |
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/6-31G(2df,p)
| 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' |
3696 |
3566 |
50.24 |
|
|
|
| 2 |
A' |
2809 |
2710 |
146.36 |
|
|
|
| 3 |
A' |
1519 |
1466 |
20.53 |
|
|
|
| 4 |
A' |
1335 |
1288 |
52.30 |
|
|
|
| 5 |
A' |
1217 |
1175 |
130.96 |
|
|
|
| 6 |
A" |
1096 |
1058 |
105.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5835.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 5631.6 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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.744 |
0.000 |
| O2 |
0.011 |
-0.570 |
0.000 |
| H3 |
-1.090 |
0.968 |
0.000 |
| H4 |
0.932 |
-0.874 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3136 | 1.1234 | 1.8611 |
O2 | 1.3136 | | 1.8912 | 0.9695 | H3 | 1.1234 | 1.8912 | | 2.7346 | H4 | 1.8611 | 0.9695 | 2.7346 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.260 |
|
O2 |
C1 |
H3 |
101.512 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.212 |
|
|
|
| 2 |
O |
-0.221 |
|
|
|
| 3 |
H |
0.107 |
|
|
|
| 4 |
H |
0.326 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.338 |
-1.643 |
0.000 |
1.678 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.814 |
-3.329 |
0.000 |
| y |
-3.329 |
-13.420 |
0.000 |
| z |
0.000 |
0.000 |
-11.683 |
|
| Traceless |
| | x | y | z |
| x |
1.737 |
-3.329 |
0.000 |
| y |
-3.329 |
-2.171 |
0.000 |
| z |
0.000 |
0.000 |
0.434 |
|
| Polar |
| 3z2-r2 | 0.867 |
| x2-y2 | 2.605 |
| xy | -3.329 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.530 |
-0.584 |
0.000 |
| y |
-0.584 |
2.521 |
0.000 |
| z |
0.000 |
0.000 |
1.597 |
<r2> (average value of r
2) Å
2
| <r2> |
17.153 |
| (<r2>)1/2 |
4.142 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -114.418489 |
| Energy at 298.15K | -114.419892 |
| HF Energy | -114.418489 |
| Nuclear repulsion energy | 30.636346 |
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/6-31G(2df,p)
| 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' |
3526 |
3403 |
20.33 |
|
|
|
| 2 |
A' |
2735 |
2639 |
205.39 |
|
|
|
| 3 |
A' |
1484 |
1433 |
47.72 |
|
|
|
| 4 |
A' |
1349 |
1302 |
50.46 |
|
|
|
| 5 |
A' |
1217 |
1175 |
31.12 |
|
|
|
| 6 |
A" |
1022 |
986 |
31.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5666.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 5468.6 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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.742 |
0.000 |
| O2 |
0.122 |
-0.565 |
0.000 |
| H3 |
-0.957 |
1.068 |
0.000 |
| H4 |
-0.755 |
-0.996 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3068 | 1.1276 | 1.9460 |
O2 | 1.3068 | | 1.9579 | 0.9768 | H3 | 1.1276 | 1.9579 | | 2.0740 | H4 | 1.9460 | 0.9768 | 2.0740 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
116.153 |
|
O2 |
C1 |
H3 |
106.845 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.171 |
|
|
|
| 2 |
O |
-0.219 |
|
|
|
| 3 |
H |
0.082 |
|
|
|
| 4 |
H |
0.307 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.709 |
-1.693 |
0.000 |
3.194 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.983 |
-0.024 |
0.000 |
| y |
-0.024 |
-12.892 |
0.000 |
| z |
0.000 |
0.000 |
-11.669 |
|
| Traceless |
| | x | y | z |
| x |
0.297 |
-0.024 |
0.000 |
| y |
-0.024 |
-1.066 |
0.000 |
| z |
0.000 |
0.000 |
0.768 |
|
| Polar |
| 3z2-r2 | 1.537 |
| x2-y2 | 0.909 |
| xy | -0.024 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.396 |
-0.047 |
0.000 |
| y |
-0.047 |
2.954 |
0.000 |
| z |
0.000 |
0.000 |
1.612 |
<r2> (average value of r
2) Å
2
| <r2> |
17.291 |
| (<r2>)1/2 |
4.158 |