Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -151.812881 |
| Energy at 298.15K | |
| HF Energy | -151.812881 |
| Nuclear repulsion energy | 51.903049 |
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 |
Σ |
3531 |
3368 |
96.93 |
49.82 |
0.21 |
0.35 |
| 2 |
Σ |
2055 |
1960 |
87.92 |
0.25 |
0.71 |
0.83 |
| 3 |
Σ |
1270 |
1212 |
30.70 |
31.03 |
0.27 |
0.42 |
| 4 |
Π |
521 |
497 |
35.72 |
0.75 |
0.75 |
0.86 |
| 4 |
Π |
512 |
489 |
1.87 |
1.19 |
0.75 |
0.86 |
| 5 |
Π |
468 |
446 |
0.08 |
0.95 |
0.75 |
0.86 |
| 5 |
Π |
175 |
167 |
159.32 |
5.88 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4266.6 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 4069.1 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 C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.007 |
| C2 |
0.000 |
0.000 |
-1.250 |
| O3 |
0.000 |
0.000 |
1.222 |
| H4 |
0.000 |
0.000 |
-2.312 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2565 | 1.2150 | 2.3182 |
C2 | 1.2565 | | 2.4715 | 1.0617 | O3 | 1.2150 | 2.4715 | | 3.5332 | H4 | 2.3182 | 1.0617 | 3.5332 | |
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 B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.120 |
|
|
|
| 2 |
C |
-0.056 |
|
|
|
| 3 |
O |
-0.335 |
|
|
|
| 4 |
H |
0.270 |
|
|
|
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 |
-2.492 |
2.492 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.882 |
0.000 |
0.000 |
| y |
0.000 |
-17.489 |
0.000 |
| z |
0.000 |
0.000 |
-15.074 |
|
| Traceless |
| | x | y | z |
| x |
0.400 |
0.000 |
0.000 |
| y |
0.000 |
-2.011 |
0.000 |
| z |
0.000 |
0.000 |
1.611 |
|
| Polar |
| 3z2-r2 | 3.223 |
| x2-y2 | 1.607 |
| 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 |
1.235 |
0.000 |
0.000 |
| y |
0.000 |
1.168 |
0.000 |
| z |
0.000 |
0.000 |
5.505 |
<r2> (average value of r
2) Å
2
| <r2> |
36.741 |
| (<r2>)1/2 |
6.061 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -151.812881 |
| Energy at 298.15K | |
| HF Energy | -151.812881 |
| Nuclear repulsion energy | 51.904118 |
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' |
3531 |
3367 |
96.90 |
49.82 |
0.21 |
0.35 |
| 2 |
A' |
2055 |
1960 |
87.69 |
0.25 |
0.70 |
0.83 |
| 3 |
A' |
1271 |
1212 |
30.73 |
31.04 |
0.27 |
0.42 |
| 4 |
A' |
512 |
489 |
1.94 |
1.18 |
0.75 |
0.86 |
| 5 |
A' |
178 |
170 |
159.20 |
5.92 |
0.75 |
0.85 |
| 6 |
A" |
482 |
460 |
10.86 |
1.64 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4014.3 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 3828.4 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 |
0.000 |
0.006 |
0.000 |
| C2 |
-0.005 |
-1.250 |
0.000 |
| O3 |
0.005 |
1.222 |
0.000 |
| H4 |
-0.009 |
-2.312 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2564 | 1.2150 | 2.3181 |
C2 | 1.2564 | | 2.4714 | 1.0618 | O3 | 1.2150 | 2.4714 | | 3.5332 | H4 | 2.3181 | 1.0618 | 3.5332 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
179.970 |
|
C2 |
C1 |
O3 |
180.000 |
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 |
0.120 |
|
|
|
| 2 |
C |
-0.055 |
|
|
|
| 3 |
O |
-0.335 |
|
|
|
| 4 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.009 |
-2.492 |
0.000 |
2.492 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.488 |
0.007 |
0.000 |
| y |
0.007 |
-15.074 |
0.000 |
| z |
0.000 |
0.000 |
-15.882 |
|
| Traceless |
| | x | y | z |
| x |
-2.011 |
0.007 |
0.000 |
| y |
0.007 |
1.611 |
0.000 |
| z |
0.000 |
0.000 |
0.399 |
|
| Polar |
| 3z2-r2 | 0.798 |
| x2-y2 | -2.415 |
| xy | 0.007 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.168 |
0.017 |
0.000 |
| y |
0.017 |
5.505 |
0.000 |
| z |
0.000 |
0.000 |
1.235 |
<r2> (average value of r
2) Å
2
| <r2> |
36.740 |
| (<r2>)1/2 |
6.061 |