Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -114.361100 |
| Energy at 298.15K | -114.362518 |
| HF Energy | -114.361100 |
| Nuclear repulsion energy | 30.710126 |
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 B1B95/6-31G*
| 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' |
3700 |
3513 |
52.39 |
|
|
|
| 2 |
A' |
2852 |
2707 |
171.61 |
|
|
|
| 3 |
A' |
1542 |
1464 |
33.18 |
|
|
|
| 4 |
A' |
1372 |
1302 |
77.98 |
|
|
|
| 5 |
A' |
1230 |
1168 |
122.68 |
|
|
|
| 6 |
A" |
1114 |
1057 |
121.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5904.7 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 5605.3 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.011 |
0.743 |
0.000 |
| O2 |
0.011 |
-0.569 |
0.000 |
| H3 |
-1.088 |
0.960 |
0.000 |
| H4 |
0.935 |
-0.870 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3115 | 1.1202 | 1.8586 |
O2 | 1.3115 | | 1.8828 | 0.9715 | H3 | 1.1202 | 1.8828 | | 2.7277 | H4 | 1.8586 | 0.9715 | 2.7277 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.073 |
|
O2 |
C1 |
H3 |
101.188 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.092 |
|
|
|
| 2 |
O |
-0.472 |
|
|
|
| 3 |
H |
0.119 |
|
|
|
| 4 |
H |
0.445 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.414 |
-1.617 |
0.000 |
1.669 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.745 |
-3.491 |
0.000 |
| y |
-3.491 |
-13.432 |
0.000 |
| z |
0.000 |
0.000 |
-11.625 |
|
| Traceless |
| | x | y | z |
| x |
1.784 |
-3.491 |
0.000 |
| y |
-3.491 |
-2.247 |
0.000 |
| z |
0.000 |
0.000 |
0.463 |
|
| Polar |
| 3z2-r2 | 0.926 |
| x2-y2 | 2.687 |
| xy | -3.491 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.397 |
-0.608 |
0.000 |
| y |
-0.608 |
2.335 |
0.000 |
| z |
0.000 |
0.000 |
1.336 |
<r2> (average value of r
2) Å
2
| <r2> |
17.089 |
| (<r2>)1/2 |
4.134 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -114.352780 |
| Energy at 298.15K | -114.354186 |
| HF Energy | -114.352780 |
| Nuclear repulsion energy | 30.654964 |
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 B1B95/6-31G*
| 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' |
3517 |
3339 |
22.04 |
|
|
|
| 2 |
A' |
2754 |
2614 |
248.79 |
|
|
|
| 3 |
A' |
1498 |
1422 |
54.46 |
|
|
|
| 4 |
A' |
1379 |
1309 |
68.25 |
|
|
|
| 5 |
A' |
1249 |
1186 |
29.35 |
|
|
|
| 6 |
A" |
1032 |
979 |
42.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5714.4 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 5424.7 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.122 |
0.742 |
0.000 |
| O2 |
0.122 |
-0.563 |
0.000 |
| H3 |
-0.959 |
1.060 |
0.000 |
| H4 |
-0.753 |
-1.003 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
H3 |
H4 |
| C1 | | 1.3052 | 1.1268 | 1.9519 |
O2 | 1.3052 | | 1.9505 | 0.9792 | H3 | 1.1268 | 1.9505 | | 2.0735 | H4 | 1.9519 | 0.9792 | 2.0735 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
116.679 |
|
O2 |
C1 |
H3 |
106.415 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.038 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
H |
0.085 |
|
|
|
| 4 |
H |
0.417 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.919 |
-1.702 |
0.000 |
3.379 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.031 |
0.100 |
0.000 |
| y |
0.100 |
-12.864 |
0.000 |
| z |
0.000 |
0.000 |
-11.604 |
|
| Traceless |
| | x | y | z |
| x |
0.203 |
0.100 |
0.000 |
| y |
0.100 |
-1.047 |
0.000 |
| z |
0.000 |
0.000 |
0.844 |
|
| Polar |
| 3z2-r2 | 1.687 |
| x2-y2 | 0.834 |
| xy | 0.100 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.271 |
-0.079 |
0.000 |
| y |
-0.079 |
2.788 |
0.000 |
| z |
0.000 |
0.000 |
1.359 |
<r2> (average value of r
2) Å
2
| <r2> |
17.264 |
| (<r2>)1/2 |
4.155 |