Jump to
S1C2
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -113.858854 |
| Energy at 298.15K | -113.860264 |
| HF Energy | -113.858854 |
| Nuclear repulsion energy | 30.816621 |
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 LSDA/TZVP
| 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' |
3556 |
3514 |
61.37 |
|
|
|
| 2 |
A' |
2761 |
2729 |
134.72 |
|
|
|
| 3 |
A' |
1451 |
1434 |
18.58 |
|
|
|
| 4 |
A' |
1355 |
1339 |
73.46 |
|
|
|
| 5 |
A' |
1156 |
1143 |
101.92 |
|
|
|
| 6 |
A" |
1105 |
1092 |
123.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5692.2 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 5626.2 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 LSDA/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.737 |
0.000 |
| O2 |
0.011 |
-0.563 |
0.000 |
| H3 |
-1.093 |
0.966 |
0.000 |
| H4 |
0.938 |
-0.885 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.2991 | 1.1277 | 1.8682 |
O2 | 1.2991 | | 1.8858 | 0.9818 | H3 | 1.1277 | 1.8858 | | 2.7485 | H4 | 1.8682 | 0.9818 | 2.7485 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.194 |
|
O2 |
C1 |
H3 |
101.751 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.231 |
|
|
|
| 2 |
O |
-0.219 |
|
|
|
| 3 |
H |
0.111 |
|
|
|
| 4 |
H |
0.340 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.231 |
-1.899 |
0.000 |
1.913 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.351 |
-3.975 |
0.000 |
| y |
-3.975 |
-14.207 |
0.000 |
| z |
0.000 |
0.000 |
-12.360 |
|
| Traceless |
| | x | y | z |
| x |
1.932 |
-3.975 |
0.000 |
| y |
-3.975 |
-2.351 |
0.000 |
| z |
0.000 |
0.000 |
0.419 |
|
| Polar |
| 3z2-r2 | 0.837 |
| x2-y2 | 2.856 |
| xy | -3.975 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.019 |
-0.508 |
0.000 |
| y |
-0.508 |
2.969 |
0.000 |
| z |
0.000 |
0.000 |
1.941 |
<r2> (average value of r
2) Å
2
| <r2> |
17.475 |
| (<r2>)1/2 |
4.180 |
Jump to
S1C1
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -113.849483 |
| Energy at 298.15K | -113.850876 |
| HF Energy | -113.849483 |
| Nuclear repulsion energy | 30.744178 |
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 LSDA/TZVP
| 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' |
3240 |
3202 |
110.42 |
|
|
|
| 2 |
A' |
2657 |
2626 |
221.17 |
|
|
|
| 3 |
A' |
1411 |
1395 |
76.54 |
|
|
|
| 4 |
A' |
1362 |
1346 |
22.63 |
|
|
|
| 5 |
A' |
1131 |
1118 |
14.98 |
|
|
|
| 6 |
A" |
1019 |
1007 |
35.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5409.8 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 5347.0 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 LSDA/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.734 |
0.000 |
| O2 |
0.122 |
-0.557 |
0.000 |
| H3 |
-0.959 |
1.076 |
0.000 |
| H4 |
-0.755 |
-1.027 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.2914 | 1.1343 | 1.9682 |
O2 | 1.2914 | | 1.9586 | 0.9957 | H3 | 1.1343 | 1.9586 | | 2.1127 | H4 | 1.9682 | 0.9957 | 2.1127 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
118.176 |
|
O2 |
C1 |
H3 |
107.509 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.141 |
|
|
|
| 2 |
O |
-0.212 |
|
|
|
| 3 |
H |
0.078 |
|
|
|
| 4 |
H |
0.276 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.166 |
-1.885 |
0.000 |
3.685 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.806 |
-0.160 |
0.000 |
| y |
-0.160 |
-13.594 |
0.000 |
| z |
0.000 |
0.000 |
-12.243 |
|
| Traceless |
| | x | y | z |
| x |
0.113 |
-0.160 |
0.000 |
| y |
-0.160 |
-1.070 |
0.000 |
| z |
0.000 |
0.000 |
0.957 |
|
| Polar |
| 3z2-r2 | 1.914 |
| x2-y2 | 0.788 |
| xy | -0.160 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.033 |
0.154 |
0.000 |
| y |
0.154 |
3.795 |
0.000 |
| z |
0.000 |
0.000 |
1.900 |
<r2> (average value of r
2) Å
2
| <r2> |
17.677 |
| (<r2>)1/2 |
4.204 |