Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.818294 |
| Energy at 298.15K | |
| HF Energy | -151.818294 |
| Nuclear repulsion energy | 52.756114 |
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 HSEh1PBE/6-311+G(3df,2p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3474 |
3474 |
123.68 |
48.69 |
0.23 |
0.37 |
| 2 |
Σ |
2131 |
2131 |
277.14 |
10.77 |
0.49 |
0.66 |
| 3 |
Σ |
1327 |
1327 |
21.34 |
45.31 |
0.14 |
0.25 |
| 4 |
Π |
581 |
581 |
0.36 |
0.21 |
0.75 |
0.86 |
| 4 |
Π |
539 |
539 |
9.73 |
0.66 |
0.75 |
0.86 |
| 5 |
Π |
439 |
439 |
22.42 |
0.31 |
0.75 |
0.86 |
| 5 |
Π |
338i |
338i |
122.71 |
7.18 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4075.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4075.7 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.022 |
| C2 |
0.000 |
0.000 |
-1.236 |
| O3 |
0.000 |
0.000 |
1.198 |
| H4 |
0.000 |
0.000 |
-2.298 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2572 | 1.1762 | 2.3192 |
C2 | 1.2572 | | 2.4334 | 1.0621 | O3 | 1.1762 | 2.4334 | | 3.4955 | H4 | 2.3192 | 1.0621 | 3.4955 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
180.000 |
|
C2 |
C1 |
O3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.588 |
|
|
|
| 2 |
C |
-0.193 |
|
|
|
| 3 |
O |
-0.632 |
|
|
|
| 4 |
H |
0.238 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.129 |
2.129 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.245 |
0.000 |
0.000 |
| y |
0.000 |
-18.042 |
0.000 |
| z |
0.000 |
0.000 |
-14.876 |
|
| Traceless |
| | x | y | z |
| x |
0.214 |
0.000 |
0.000 |
| y |
0.000 |
-2.481 |
0.000 |
| z |
0.000 |
0.000 |
2.267 |
|
| Polar |
| 3z2-r2 | 4.534 |
| x2-y2 | 1.796 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.624 |
0.000 |
0.000 |
| y |
0.000 |
2.963 |
0.000 |
| z |
0.000 |
0.000 |
6.191 |
<r2> (average value of r
2) Å
2
| <r2> |
36.156 |
| (<r2>)1/2 |
6.013 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.820139 |
| Energy at 298.15K | |
| HF Energy | -151.820139 |
| Nuclear repulsion energy | 52.636364 |
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 HSEh1PBE/6-311+G(3df,2p)
| 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' |
3358 |
3358 |
51.04 |
71.44 |
0.31 |
0.48 |
| 2 |
A' |
2126 |
2126 |
358.62 |
8.45 |
0.72 |
0.84 |
| 3 |
A' |
1279 |
1279 |
5.29 |
38.80 |
0.16 |
0.28 |
| 4 |
A' |
577 |
577 |
7.82 |
3.56 |
0.69 |
0.82 |
| 5 |
A' |
463 |
463 |
234.93 |
1.57 |
0.15 |
0.26 |
| 6 |
A" |
513 |
513 |
3.41 |
0.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4157.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4157.5 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.045 |
0.000 |
| C2 |
1.010 |
-0.753 |
0.000 |
| O3 |
-1.018 |
0.614 |
0.000 |
| H4 |
2.079 |
-0.672 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2876 | 1.1659 | 2.1992 |
C2 | 1.2876 | | 2.4458 | 1.0716 | O3 | 1.1659 | 2.4458 | | 3.3531 | H4 | 2.1992 | 1.0716 | 3.3531 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
137.370 |
|
C2 |
C1 |
O3 |
170.903 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.721 |
|
|
|
| 2 |
C |
-0.353 |
|
|
|
| 3 |
O |
-0.569 |
|
|
|
| 4 |
H |
0.201 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.669 |
0.195 |
0.000 |
1.680 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.118 |
0.514 |
0.000 |
| y |
0.514 |
-19.243 |
0.000 |
| z |
0.000 |
0.000 |
-16.379 |
|
| Traceless |
| | x | y | z |
| x |
2.693 |
0.514 |
0.000 |
| y |
0.514 |
-3.495 |
0.000 |
| z |
0.000 |
0.000 |
0.802 |
|
| Polar |
| 3z2-r2 | 1.603 |
| x2-y2 | 4.125 |
| xy | 0.514 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.097 |
-1.567 |
0.000 |
| y |
-1.567 |
4.221 |
0.000 |
| z |
0.000 |
0.000 |
3.032 |
<r2> (average value of r
2) Å
2
| <r2> |
36.179 |
| (<r2>)1/2 |
6.015 |