Jump to
S1C2
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -113.755890 |
| Energy at 298.15K | -113.757282 |
| HF Energy | -113.755890 |
| Nuclear repulsion energy | 29.971453 |
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/6-31G
| 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' |
3447 |
3377 |
31.32 |
|
|
|
| 2 |
A' |
2690 |
2635 |
174.78 |
|
|
|
| 3 |
A' |
1453 |
1424 |
28.83 |
|
|
|
| 4 |
A' |
1235 |
1209 |
33.50 |
|
|
|
| 5 |
A' |
1132 |
1109 |
169.18 |
|
|
|
| 6 |
A" |
1078 |
1056 |
163.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5517.1 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5405.1 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 LSDA/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.012 |
0.765 |
0.000 |
| O2 |
0.012 |
-0.579 |
0.000 |
| H3 |
-1.109 |
0.981 |
0.000 |
| H4 |
0.939 |
-0.936 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3443 | 1.1422 | 1.9366 |
O2 | 1.3443 | | 1.9218 | 0.9925 | H3 | 1.1422 | 1.9218 | | 2.8052 | H4 | 1.9366 | 0.9925 | 2.8052 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
111.049 |
|
O2 |
C1 |
H3 |
100.918 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.070 |
|
|
|
| 2 |
O |
-0.483 |
|
|
|
| 3 |
H |
0.130 |
|
|
|
| 4 |
H |
0.423 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.504 |
-1.696 |
0.000 |
1.769 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.950 |
-4.089 |
0.000 |
| y |
-4.089 |
-13.712 |
0.000 |
| z |
0.000 |
0.000 |
-11.868 |
|
| Traceless |
| | x | y | z |
| x |
1.840 |
-4.089 |
0.000 |
| y |
-4.089 |
-2.303 |
0.000 |
| z |
0.000 |
0.000 |
0.463 |
|
| Polar |
| 3z2-r2 | 0.925 |
| x2-y2 | 2.762 |
| xy | -4.089 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.521 |
-0.707 |
0.000 |
| y |
-0.707 |
2.470 |
0.000 |
| z |
0.000 |
0.000 |
1.280 |
<r2> (average value of r
2) Å
2
| <r2> |
17.753 |
| (<r2>)1/2 |
4.213 |
Jump to
S1C1
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -113.747067 |
| Energy at 298.15K | -113.748446 |
| HF Energy | -113.747067 |
| Nuclear repulsion energy | 29.989932 |
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/6-31G
| 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' |
2940 |
2880 |
275.85 |
|
|
|
| 2 |
A' |
2527 |
2476 |
305.51 |
|
|
|
| 3 |
A' |
1378 |
1350 |
118.18 |
|
|
|
| 4 |
A' |
1281 |
1255 |
4.21 |
|
|
|
| 5 |
A' |
1113 |
1091 |
24.40 |
|
|
|
| 6 |
A" |
1010 |
990 |
48.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5124.5 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5020.4 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 LSDA/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.757 |
0.000 |
| O2 |
0.122 |
-0.567 |
0.000 |
| H3 |
-0.976 |
1.111 |
0.000 |
| H4 |
-0.734 |
-1.117 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3236 | 1.1540 | 2.0599 |
O2 | 1.3236 | | 2.0053 | 1.0176 | H3 | 1.1540 | 2.0053 | | 2.2408 | H4 | 2.0599 | 1.0176 | 2.2408 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
122.707 |
|
O2 |
C1 |
H3 |
107.875 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.012 |
|
|
|
| 2 |
O |
-0.470 |
|
|
|
| 3 |
H |
0.090 |
|
|
|
| 4 |
H |
0.368 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.264 |
-1.670 |
0.000 |
3.667 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.632 |
0.136 |
0.000 |
| y |
0.136 |
-12.967 |
0.000 |
| z |
0.000 |
0.000 |
-11.850 |
|
| Traceless |
| | x | y | z |
| x |
-0.223 |
0.136 |
0.000 |
| y |
0.136 |
-0.726 |
0.000 |
| z |
0.000 |
0.000 |
0.949 |
|
| Polar |
| 3z2-r2 | 1.898 |
| x2-y2 | 0.335 |
| xy | 0.136 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.447 |
0.221 |
0.000 |
| y |
0.221 |
3.677 |
0.000 |
| z |
0.000 |
0.000 |
1.315 |
<r2> (average value of r
2) Å
2
| <r2> |
17.985 |
| (<r2>)1/2 |
4.241 |