Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -114.417975 |
Energy at 298.15K | -114.419382 |
HF Energy | -114.417975 |
Nuclear repulsion energy | 30.335538 |
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 BLYP/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' |
3501 |
3492 |
25.05 |
|
|
|
2 |
A' |
2723 |
2716 |
189.85 |
|
|
|
3 |
A' |
1506 |
1503 |
24.74 |
|
|
|
4 |
A' |
1258 |
1255 |
11.36 |
|
|
|
5 |
A' |
1192 |
1189 |
157.30 |
|
|
|
6 |
A" |
1101 |
1098 |
124.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5640.9 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 5626.8 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.011 |
0.754 |
0.000 |
O2 |
0.011 |
-0.576 |
0.000 |
H3 |
-1.096 |
0.968 |
0.000 |
H4 |
0.941 |
-0.888 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.3297 | 1.1279 | 1.8872 |
O2 | 1.3297 | | 1.8997 | 0.9810 | H3 | 1.1279 | 1.8997 | | 2.7560 | H4 | 1.8872 | 0.9810 | 2.7560 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
108.572 |
|
O2 |
C1 |
H3 |
100.924 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.196 |
|
|
|
2 |
O |
-0.357 |
|
|
|
3 |
H |
0.155 |
|
|
|
4 |
H |
0.398 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.352 |
-1.693 |
0.000 |
1.729 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-11.109 |
-3.687 |
0.000 |
y |
-3.687 |
-13.816 |
0.000 |
z |
0.000 |
0.000 |
-12.043 |
|
Traceless |
| x | y | z |
x |
1.821 |
-3.687 |
0.000 |
y |
-3.687 |
-2.240 |
0.000 |
z |
0.000 |
0.000 |
0.419 |
|
Polar |
3z2-r2 | 0.838 |
x2-y2 | 2.708 |
xy | -3.687 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.648 |
-0.599 |
0.000 |
y |
-0.599 |
2.625 |
0.000 |
z |
0.000 |
0.000 |
1.536 |
<r2> (average value of r
2) Å
2
<r2> |
17.574 |
(<r2>)1/2 |
4.192 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -114.410000 |
Energy at 298.15K | -114.411392 |
HF Energy | -114.410000 |
Nuclear repulsion energy | 30.311606 |
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 BLYP/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' |
3150 |
3142 |
150.16 |
|
|
|
2 |
A' |
2611 |
2604 |
294.49 |
|
|
|
3 |
A' |
1452 |
1449 |
63.25 |
|
|
|
4 |
A' |
1279 |
1276 |
21.49 |
|
|
|
5 |
A' |
1178 |
1175 |
22.42 |
|
|
|
6 |
A" |
1016 |
1014 |
35.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5343.1 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 5329.8 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.123 |
0.749 |
0.000 |
O2 |
0.123 |
-0.568 |
0.000 |
H3 |
-0.961 |
1.085 |
0.000 |
H4 |
-0.761 |
-1.031 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
H3 |
H4 |
C1 | | 1.3171 | 1.1353 | 1.9871 |
O2 | 1.3171 | | 1.9772 | 0.9979 | H3 | 1.1353 | 1.9772 | | 2.1251 | H4 | 1.9871 | 0.9979 | 2.1251 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H4 |
117.602 |
|
O2 |
C1 |
H3 |
107.223 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.144 |
|
|
|
2 |
O |
-0.344 |
|
|
|
3 |
H |
0.129 |
|
|
|
4 |
H |
0.359 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.987 |
-1.685 |
0.000 |
3.429 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-12.511 |
-0.040 |
0.000 |
y |
-0.040 |
-13.256 |
0.000 |
z |
0.000 |
0.000 |
-11.995 |
|
Traceless |
| x | y | z |
x |
0.115 |
-0.040 |
0.000 |
y |
-0.040 |
-1.003 |
0.000 |
z |
0.000 |
0.000 |
0.888 |
|
Polar |
3z2-r2 | 1.777 |
x2-y2 | 0.746 |
xy | -0.040 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.619 |
0.112 |
0.000 |
y |
0.112 |
3.436 |
0.000 |
z |
0.000 |
0.000 |
1.526 |
<r2> (average value of r
2) Å
2
<r2> |
17.765 |
(<r2>)1/2 |
4.215 |