Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -192.946223 |
| Energy at 298.15K | -192.953500 |
| HF Energy | -192.946223 |
| Nuclear repulsion energy | 128.617795 |
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/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3097 |
2974 |
26.78 |
|
|
|
| 2 |
A1 |
3041 |
2921 |
2.28 |
|
|
|
| 3 |
A1 |
1547 |
1486 |
0.00 |
|
|
|
| 4 |
A1 |
1489 |
1430 |
5.14 |
|
|
|
| 5 |
A1 |
1393 |
1338 |
1.57 |
|
|
|
| 6 |
A1 |
1076 |
1033 |
9.03 |
|
|
|
| 7 |
A1 |
960 |
922 |
31.66 |
|
|
|
| 8 |
A1 |
822 |
789 |
3.93 |
|
|
|
| 9 |
A2 |
3079 |
2957 |
0.00 |
|
|
|
| 10 |
A2 |
1242 |
1193 |
0.00 |
|
|
|
| 11 |
A2 |
1173 |
1127 |
0.00 |
|
|
|
| 12 |
A2 |
845 |
812 |
0.00 |
|
|
|
| 13 |
B1 |
3155 |
3030 |
33.22 |
|
|
|
| 14 |
B1 |
3078 |
2956 |
84.81 |
|
|
|
| 15 |
B1 |
1203 |
1156 |
0.18 |
|
|
|
| 16 |
B1 |
1158 |
1113 |
2.87 |
|
|
|
| 17 |
B1 |
771 |
741 |
0.31 |
|
|
|
| 18 |
B1 |
74 |
71 |
2.66 |
|
|
|
| 19 |
B2 |
3030 |
2910 |
160.59 |
|
|
|
| 20 |
B2 |
1517 |
1457 |
1.13 |
|
|
|
| 21 |
B2 |
1324 |
1272 |
0.16 |
|
|
|
| 22 |
B2 |
1272 |
1221 |
13.27 |
|
|
|
| 23 |
B2 |
1075 |
1032 |
102.37 |
|
|
|
| 24 |
B2 |
970 |
932 |
4.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19194.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 18434.6 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/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.066 |
| C2 |
0.000 |
0.000 |
-1.072 |
| C3 |
0.000 |
1.030 |
0.065 |
| C4 |
0.000 |
-1.030 |
0.065 |
| H5 |
0.890 |
0.000 |
-1.701 |
| H6 |
-0.890 |
0.000 |
-1.701 |
| H7 |
0.892 |
1.662 |
0.132 |
| H8 |
-0.892 |
1.662 |
0.132 |
| H9 |
-0.892 |
-1.662 |
0.132 |
| H10 |
0.892 |
-1.662 |
0.132 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1377 | 1.4359 | 1.4359 | 2.9069 | 2.9069 | 2.1048 | 2.1048 | 2.1048 | 2.1048 |
C2 | 2.1377 | | 1.5337 | 1.5337 | 1.0902 | 1.0902 | 2.2379 | 2.2379 | 2.2379 | 2.2379 | C3 | 1.4359 | 1.5337 | | 2.0590 | 2.2299 | 2.2299 | 1.0956 | 1.0956 | 2.8364 | 2.8364 | C4 | 1.4359 | 1.5337 | 2.0590 | | 2.2299 | 2.2299 | 2.8364 | 2.8364 | 1.0956 | 1.0956 | H5 | 2.9069 | 1.0902 | 2.2299 | 2.2299 | | 1.7802 | 2.4748 | 3.0496 | 3.0496 | 2.4748 | H6 | 2.9069 | 1.0902 | 2.2299 | 2.2299 | 1.7802 | | 3.0496 | 2.4748 | 2.4748 | 3.0496 | H7 | 2.1048 | 2.2379 | 1.0956 | 2.8364 | 2.4748 | 3.0496 | | 1.7839 | 3.7728 | 3.3244 | H8 | 2.1048 | 2.2379 | 1.0956 | 2.8364 | 3.0496 | 2.4748 | 1.7839 | | 3.3244 | 3.7728 | H9 | 2.1048 | 2.2379 | 2.8364 | 1.0956 | 3.0496 | 2.4748 | 3.7728 | 3.3244 | | 1.7839 | H10 | 2.1048 | 2.2379 | 2.8364 | 1.0956 | 2.4748 | 3.0496 | 3.3244 | 3.7728 | 1.7839 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.028 |
|
O1 |
C3 |
H7 |
111.798 |
| O1 |
C3 |
H8 |
111.798 |
|
O1 |
C4 |
C2 |
92.028 |
| O1 |
C4 |
H9 |
111.798 |
|
O1 |
C4 |
H10 |
111.798 |
| C2 |
C3 |
H7 |
115.660 |
|
C2 |
C3 |
H8 |
115.660 |
| C2 |
C4 |
H9 |
115.660 |
|
C2 |
C4 |
H10 |
115.660 |
| C3 |
O1 |
C4 |
91.616 |
|
C3 |
C2 |
C4 |
84.327 |
| C3 |
C2 |
H5 |
115.342 |
|
C3 |
C2 |
H6 |
115.342 |
| C4 |
C2 |
H5 |
115.342 |
|
C4 |
C2 |
H6 |
115.342 |
| H5 |
C2 |
H6 |
109.457 |
|
H7 |
C3 |
H8 |
109.002 |
| H9 |
C4 |
H10 |
109.002 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.367 |
|
|
|
| 2 |
C |
-0.397 |
|
|
|
| 3 |
C |
0.022 |
|
|
|
| 4 |
C |
0.022 |
|
|
|
| 5 |
H |
0.141 |
|
|
|
| 6 |
H |
0.141 |
|
|
|
| 7 |
H |
0.109 |
|
|
|
| 8 |
H |
0.109 |
|
|
|
| 9 |
H |
0.109 |
|
|
|
| 10 |
H |
0.109 |
|
|
|
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 |
-1.936 |
1.936 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.052 |
0.000 |
0.000 |
| y |
0.000 |
-22.914 |
0.000 |
| z |
0.000 |
0.000 |
-27.755 |
|
| Traceless |
| | x | y | z |
| x |
1.283 |
0.000 |
0.000 |
| y |
0.000 |
2.989 |
0.000 |
| z |
0.000 |
0.000 |
-4.272 |
|
| Polar |
| 3z2-r2 | -8.544 |
| x2-y2 | -1.137 |
| 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 |
4.844 |
0.000 |
0.000 |
| y |
0.000 |
5.874 |
0.000 |
| z |
0.000 |
0.000 |
4.845 |
<r2> (average value of r
2) Å
2
| <r2> |
65.986 |
| (<r2>)1/2 |
8.123 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -192.946223 |
| Energy at 298.15K | -192.953500 |
| HF Energy | -192.946223 |
| Nuclear repulsion energy | 128.617935 |
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/6-311G**
| 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' |
3155 |
3030 |
33.28 |
|
|
|
| 2 |
A' |
3097 |
2974 |
26.79 |
|
|
|
| 3 |
A' |
3078 |
2956 |
84.75 |
|
|
|
| 4 |
A' |
3041 |
2921 |
2.29 |
|
|
|
| 5 |
A' |
1547 |
1486 |
0.00 |
|
|
|
| 6 |
A' |
1489 |
1430 |
5.14 |
|
|
|
| 7 |
A' |
1393 |
1338 |
1.57 |
|
|
|
| 8 |
A' |
1203 |
1156 |
0.18 |
|
|
|
| 9 |
A' |
1158 |
1113 |
2.87 |
|
|
|
| 10 |
A' |
1076 |
1033 |
9.04 |
|
|
|
| 11 |
A' |
960 |
922 |
31.65 |
|
|
|
| 12 |
A' |
822 |
789 |
3.93 |
|
|
|
| 13 |
A' |
771 |
741 |
0.31 |
|
|
|
| 14 |
A' |
74 |
71 |
2.66 |
|
|
|
| 15 |
A" |
3079 |
2957 |
0.00 |
|
|
|
| 16 |
A" |
3030 |
2910 |
160.58 |
|
|
|
| 17 |
A" |
1517 |
1457 |
1.13 |
|
|
|
| 18 |
A" |
1324 |
1272 |
0.16 |
|
|
|
| 19 |
A" |
1272 |
1221 |
13.26 |
|
|
|
| 20 |
A" |
1242 |
1193 |
0.00 |
|
|
|
| 21 |
A" |
1173 |
1127 |
0.00 |
|
|
|
| 22 |
A" |
1075 |
1032 |
102.38 |
|
|
|
| 23 |
A" |
970 |
932 |
4.39 |
|
|
|
| 24 |
A" |
845 |
812 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19194.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 18434.6 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
-1.066 |
0.000 |
| C2 |
-0.000 |
1.072 |
0.000 |
| C3 |
0.000 |
-0.065 |
1.030 |
| C4 |
0.000 |
-0.065 |
-1.030 |
| H5 |
0.890 |
1.702 |
0.000 |
| H6 |
-0.890 |
1.701 |
0.000 |
| H7 |
0.892 |
-0.132 |
1.662 |
| H8 |
-0.892 |
-0.132 |
1.662 |
| H9 |
0.892 |
-0.132 |
-1.662 |
| H10 |
-0.892 |
-0.132 |
-1.662 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1377 | 1.4358 | 1.4358 | 2.9071 | 2.9069 | 2.1048 | 2.1048 | 2.1048 | 2.1048 |
C2 | 2.1377 | | 1.5337 | 1.5337 | 1.0902 | 1.0902 | 2.2378 | 2.2378 | 2.2378 | 2.2378 | C3 | 1.4358 | 1.5337 | | 2.0590 | 2.2300 | 2.2299 | 1.0956 | 1.0956 | 2.8364 | 2.8365 | C4 | 1.4358 | 1.5337 | 2.0590 | | 2.2300 | 2.2299 | 2.8364 | 2.8365 | 1.0956 | 1.0956 | H5 | 2.9071 | 1.0902 | 2.2300 | 2.2300 | | 1.7801 | 2.4749 | 3.0496 | 2.4749 | 3.0496 | H6 | 2.9069 | 1.0902 | 2.2299 | 2.2299 | 1.7801 | | 3.0497 | 2.4748 | 3.0497 | 2.4748 | H7 | 2.1048 | 2.2378 | 1.0956 | 2.8364 | 2.4749 | 3.0497 | | 1.7840 | 3.3241 | 3.7727 | H8 | 2.1048 | 2.2378 | 1.0956 | 2.8365 | 3.0496 | 2.4748 | 1.7840 | | 3.7727 | 3.3245 | H9 | 2.1048 | 2.2378 | 2.8364 | 1.0956 | 2.4749 | 3.0497 | 3.3241 | 3.7727 | | 1.7840 | H10 | 2.1048 | 2.2378 | 2.8365 | 1.0956 | 3.0496 | 2.4748 | 3.7727 | 3.3245 | 1.7840 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.028 |
|
O1 |
C3 |
H7 |
111.797 |
| O1 |
C3 |
H8 |
111.799 |
|
O1 |
C4 |
C2 |
92.028 |
| O1 |
C4 |
H9 |
111.797 |
|
O1 |
C4 |
H10 |
111.799 |
| C2 |
C3 |
H7 |
115.658 |
|
C2 |
C3 |
H8 |
115.656 |
| C2 |
C4 |
H9 |
115.658 |
|
C2 |
C4 |
H10 |
115.656 |
| C3 |
O1 |
C4 |
91.617 |
|
C3 |
C2 |
C4 |
84.326 |
| C3 |
C2 |
H5 |
115.348 |
|
C3 |
C2 |
H6 |
115.343 |
| C4 |
C2 |
H5 |
115.348 |
|
C4 |
C2 |
H6 |
115.343 |
| H5 |
C2 |
H6 |
109.448 |
|
H7 |
C3 |
H8 |
109.005 |
| H9 |
C4 |
H10 |
109.005 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.367 |
|
|
|
| 2 |
C |
-0.397 |
|
|
|
| 3 |
C |
0.022 |
|
|
|
| 4 |
C |
0.022 |
|
|
|
| 5 |
H |
0.141 |
|
|
|
| 6 |
H |
0.141 |
|
|
|
| 7 |
H |
0.109 |
|
|
|
| 8 |
H |
0.109 |
|
|
|
| 9 |
H |
0.109 |
|
|
|
| 10 |
H |
0.109 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.000 |
1.936 |
0.000 |
1.936 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.052 |
0.000 |
0.000 |
| y |
0.000 |
-27.755 |
0.000 |
| z |
0.000 |
0.000 |
-22.915 |
|
| Traceless |
| | x | y | z |
| x |
1.283 |
0.000 |
0.000 |
| y |
0.000 |
-4.271 |
0.000 |
| z |
0.000 |
0.000 |
2.988 |
|
| Polar |
| 3z2-r2 | 5.977 |
| x2-y2 | 3.703 |
| 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 |
4.844 |
0.000 |
0.000 |
| y |
0.000 |
4.845 |
0.000 |
| z |
0.000 |
0.000 |
5.874 |
<r2> (average value of r
2) Å
2
| <r2> |
65.986 |
| (<r2>)1/2 |
8.123 |