Jump to
S2C1
Energy calculated at mPW1PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -77.262643 |
| Energy at 298.15K | -77.262275 |
| Nuclear repulsion energy | 23.974968 |
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 mPW1PW91/cc-pVTZ
| 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 |
3143 |
3014 |
50.03 |
|
|
|
| 2 |
A1 |
1728 |
1657 |
90.63 |
|
|
|
| 3 |
A1 |
1210 |
1160 |
26.60 |
|
|
|
| 4 |
B1 |
753 |
722 |
80.23 |
|
|
|
| 5 |
B2 |
3226 |
3094 |
22.64 |
|
|
|
| 6 |
B2 |
288 |
276 |
6.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5173.3 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 4962.3 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 mPW1PW91/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.475 |
| C2 |
0.000 |
0.000 |
0.815 |
| H3 |
0.000 |
0.938 |
-1.022 |
| H4 |
0.000 |
-0.938 |
-1.022 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2900 | 1.0860 | 1.0860 |
C2 | 1.2900 | | 2.0630 | 2.0630 | H3 | 1.0860 | 2.0630 | | 1.8759 | H4 | 1.0860 | 2.0630 | 1.8759 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.269 |
|
C2 |
C1 |
H4 |
120.269 |
| H3 |
C1 |
H4 |
119.463 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.260 |
|
|
|
| 2 |
C |
-0.037 |
|
|
|
| 3 |
H |
0.149 |
|
|
|
| 4 |
H |
0.149 |
|
|
|
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 |
-2.471 |
2.471 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.122 |
0.000 |
0.000 |
| y |
0.000 |
-10.299 |
0.000 |
| z |
0.000 |
0.000 |
-14.170 |
|
| Traceless |
| | x | y | z |
| x |
-1.887 |
0.000 |
0.000 |
| y |
0.000 |
3.847 |
0.000 |
| z |
0.000 |
0.000 |
-1.960 |
|
| Polar |
| 3z2-r2 | -3.920 |
| x2-y2 | -3.822 |
| 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 |
2.257 |
0.000 |
0.000 |
| y |
0.000 |
2.876 |
0.000 |
| z |
0.000 |
0.000 |
4.232 |
<r2> (average value of r
2) Å
2
| <r2> |
17.224 |
| (<r2>)1/2 |
4.150 |
Jump to
S1C1
Energy calculated at mPW1PW91/cc-pVTZ
| | hartrees |
| Energy at 0K | -77.197016 |
| Energy at 298.15K | -77.197099 |
| HF Energy | -77.197016 |
| Nuclear repulsion energy | 23.718242 |
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 mPW1PW91/cc-pVTZ
| 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 |
3057 |
2932 |
4.74 |
|
|
|
| 2 |
A1 |
1607 |
1541 |
3.57 |
|
|
|
| 3 |
A1 |
1401 |
1344 |
3.40 |
|
|
|
| 4 |
B1 |
824 |
790 |
13.88 |
|
|
|
| 5 |
B2 |
3131 |
3003 |
4.14 |
|
|
|
| 6 |
B2 |
993 |
952 |
2.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5506.0 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 5281.4 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 mPW1PW91/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.480 |
| C2 |
0.000 |
0.000 |
0.828 |
| H3 |
0.000 |
0.932 |
-1.044 |
| H4 |
0.000 |
-0.932 |
-1.044 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3075 | 1.0896 | 1.0896 |
C2 | 1.3075 | | 2.0911 | 2.0911 | H3 | 1.0896 | 2.0911 | | 1.8640 | H4 | 1.0896 | 2.0911 | 1.8640 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.216 |
|
|
|
| 2 |
C |
-0.039 |
|
|
|
| 3 |
H |
0.127 |
|
|
|
| 4 |
H |
0.127 |
|
|
|
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 |
-0.599 |
0.599 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.795 |
0.000 |
0.000 |
| y |
0.000 |
-11.980 |
0.000 |
| z |
0.000 |
0.000 |
-11.203 |
|
| Traceless |
| | x | y | z |
| x |
-2.203 |
0.000 |
0.000 |
| y |
0.000 |
0.519 |
0.000 |
| z |
0.000 |
0.000 |
1.684 |
|
| Polar |
| 3z2-r2 | 3.368 |
| x2-y2 | -1.815 |
| 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 |
2.463 |
0.000 |
0.000 |
| y |
0.000 |
2.606 |
0.000 |
| z |
0.000 |
0.000 |
4.350 |
<r2> (average value of r
2) Å
2
| <r2> |
17.109 |
| (<r2>)1/2 |
4.136 |