Jump to
S1C2
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -186.263225 |
| Energy at 298.15K | -186.264102 |
| HF Energy | -186.198722 |
| Nuclear repulsion energy | 60.217495 |
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 B2PLYP/STO-3G
| 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' |
3658 |
3658 |
18.57 |
|
|
|
| 2 |
A' |
1816 |
1816 |
52.74 |
|
|
|
| 3 |
A' |
1470 |
1470 |
0.78 |
|
|
|
| 4 |
A' |
1042 |
1042 |
68.51 |
|
|
|
| 5 |
A' |
534 |
534 |
17.22 |
|
|
|
| 6 |
A" |
500 |
500 |
67.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4509.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4509.7 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 B2PLYP/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.496 |
0.000 |
| O2 |
-1.112 |
-0.366 |
0.000 |
| O3 |
1.200 |
0.158 |
0.000 |
| H4 |
-0.704 |
-1.311 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.4067 | 1.2470 | 1.9389 |
O2 | 1.4067 | | 2.3712 | 1.0299 | O3 | 1.2470 | 2.3712 | | 2.4050 | H4 | 1.9389 | 1.0299 | 2.4050 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
104.385 |
|
O2 |
C1 |
O3 |
126.542 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.155 |
|
|
|
| 2 |
O |
-0.201 |
|
|
|
| 3 |
O |
-0.152 |
|
|
|
| 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 |
| |
-0.229 |
-1.463 |
0.000 |
1.480 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.767 |
0.360 |
0.000 |
| y |
0.360 |
-12.837 |
0.000 |
| z |
0.000 |
0.000 |
-14.064 |
|
| Traceless |
| | x | y | z |
| x |
-4.316 |
0.360 |
0.000 |
| y |
0.360 |
3.078 |
0.000 |
| z |
0.000 |
0.000 |
1.238 |
|
| Polar |
| 3z2-r2 | 2.477 |
| x2-y2 | -4.929 |
| xy | 0.360 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.971 |
0.235 |
0.000 |
| y |
0.235 |
1.458 |
0.000 |
| z |
0.000 |
0.000 |
0.484 |
<r2> (average value of r
2) Å
2
| <r2> |
35.681 |
| (<r2>)1/2 |
5.973 |
Jump to
S1C1
Energy calculated at B2PLYP/STO-3G
| | hartrees |
| Energy at 0K | -186.270528 |
| Energy at 298.15K | -186.271430 |
| HF Energy | -186.206102 |
| Nuclear repulsion energy | 59.945878 |
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 B2PLYP/STO-3G
| 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' |
3810 |
3810 |
9.17 |
|
|
|
| 2 |
A' |
1864 |
1864 |
26.02 |
|
|
|
| 3 |
A' |
1360 |
1360 |
97.09 |
|
|
|
| 4 |
A' |
1080 |
1080 |
50.13 |
|
|
|
| 5 |
A' |
565 |
565 |
2.00 |
|
|
|
| 6 |
A" |
504 |
504 |
59.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4591.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4591.3 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 B2PLYP/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.466 |
0.000 |
| O2 |
-0.985 |
-0.563 |
0.000 |
| O3 |
1.217 |
0.218 |
0.000 |
| H4 |
-1.860 |
-0.038 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.4246 | 1.2420 | 1.9271 |
O2 | 1.4246 | | 2.3361 | 1.0205 | O3 | 1.2420 | 2.3361 | | 3.0875 | H4 | 1.9271 | 1.0205 | 3.0875 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
102.773 |
|
O2 |
C1 |
O3 |
122.190 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.129 |
|
|
|
| 2 |
O |
-0.199 |
|
|
|
| 3 |
O |
-0.143 |
|
|
|
| 4 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.006 |
0.354 |
0.000 |
2.037 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.805 |
-0.989 |
0.000 |
| y |
-0.989 |
-15.646 |
0.000 |
| z |
0.000 |
0.000 |
-14.075 |
|
| Traceless |
| | x | y | z |
| x |
2.056 |
-0.989 |
0.000 |
| y |
-0.989 |
-2.206 |
0.000 |
| z |
0.000 |
0.000 |
0.151 |
|
| Polar |
| 3z2-r2 | 0.301 |
| x2-y2 | 2.841 |
| xy | -0.989 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.689 |
0.190 |
0.000 |
| y |
0.190 |
0.923 |
0.000 |
| z |
0.000 |
0.000 |
0.476 |
<r2> (average value of r
2) Å
2
| <r2> |
36.140 |
| (<r2>)1/2 |
6.012 |