Jump to
S1C2
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -188.985572 |
| Energy at 298.15K | -188.986631 |
| HF Energy | -188.985572 |
| Nuclear repulsion energy | 62.811262 |
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 PBEPBE/Def2TZVPP
| 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' |
3424 |
3383 |
6.36 |
|
|
|
| 2 |
A' |
1813 |
1791 |
287.97 |
|
|
|
| 3 |
A' |
1258 |
1243 |
0.99 |
|
|
|
| 4 |
A' |
1028 |
1016 |
123.70 |
|
|
|
| 5 |
A' |
571 |
564 |
26.45 |
|
|
|
| 6 |
A" |
589 |
582 |
92.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4341.6 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 4289.0 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 PBEPBE/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.472 |
0.000 |
| O2 |
-1.078 |
-0.343 |
0.000 |
| O3 |
1.167 |
0.146 |
0.000 |
| H4 |
-0.716 |
-1.258 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3512 | 1.2118 | 1.8722 |
O2 | 1.3512 | | 2.2973 | 0.9834 | O3 | 1.2118 | 2.2973 | | 2.3487 | H4 | 1.8722 | 0.9834 | 2.3487 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
105.548 |
|
O2 |
C1 |
O3 |
127.269 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.144 |
|
|
|
| 2 |
O |
-0.177 |
|
|
|
| 3 |
O |
-0.164 |
|
|
|
| 4 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.993 |
-1.724 |
0.000 |
1.990 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.995 |
0.762 |
0.000 |
| y |
0.762 |
-14.259 |
0.000 |
| z |
0.000 |
0.000 |
-16.410 |
|
| Traceless |
| | x | y | z |
| x |
-4.661 |
0.762 |
0.000 |
| y |
0.762 |
3.944 |
0.000 |
| z |
0.000 |
0.000 |
0.717 |
|
| Polar |
| 3z2-r2 | 1.435 |
| x2-y2 | -5.737 |
| xy | 0.762 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.851 |
0.335 |
0.000 |
| y |
0.335 |
3.406 |
0.000 |
| z |
0.000 |
0.000 |
2.100 |
<r2> (average value of r
2) Å
2
| <r2> |
35.258 |
| (<r2>)1/2 |
5.938 |
Jump to
S1C1
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -188.988515 |
| Energy at 298.15K | -188.989562 |
| HF Energy | -188.988515 |
| Nuclear repulsion energy | 62.552746 |
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 PBEPBE/Def2TZVPP
| 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' |
3688 |
3644 |
98.72 |
|
|
|
| 2 |
A' |
1843 |
1820 |
202.72 |
|
|
|
| 3 |
A' |
1199 |
1184 |
220.74 |
|
|
|
| 4 |
A' |
1058 |
1045 |
62.31 |
|
|
|
| 5 |
A' |
599 |
591 |
4.82 |
|
|
|
| 6 |
A" |
545 |
539 |
83.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4465.6 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 4411.6 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 PBEPBE/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.407 |
0.000 |
| O2 |
-0.946 |
-0.534 |
0.000 |
| O3 |
1.173 |
0.241 |
0.000 |
| H4 |
-1.816 |
-0.102 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3338 | 1.1845 | 1.8857 |
O2 | 1.3338 | | 2.2558 | 0.9714 | O3 | 1.1845 | 2.2558 | | 3.0082 | H4 | 1.8857 | 0.9714 | 3.0082 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.754 |
|
O2 |
C1 |
O3 |
127.118 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.064 |
|
|
|
| 2 |
O |
-0.148 |
|
|
|
| 3 |
O |
-0.145 |
|
|
|
| 4 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.893 |
0.198 |
0.000 |
2.900 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.929 |
-0.884 |
0.000 |
| y |
-0.884 |
-18.070 |
0.000 |
| z |
0.000 |
0.000 |
-16.472 |
|
| Traceless |
| | x | y | z |
| x |
3.342 |
-0.884 |
0.000 |
| y |
-0.884 |
-2.870 |
0.000 |
| z |
0.000 |
0.000 |
-0.473 |
|
| Polar |
| 3z2-r2 | -0.945 |
| x2-y2 | 4.141 |
| xy | -0.884 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.309 |
0.217 |
0.000 |
| y |
0.217 |
2.703 |
0.000 |
| z |
0.000 |
0.000 |
2.137 |
<r2> (average value of r
2) Å
2
| <r2> |
35.593 |
| (<r2>)1/2 |
5.966 |