Jump to
S2C1
Energy calculated at mPW1PW91/3-21G
| | hartrees |
| Energy at 0K | -76.805012 |
| Energy at 298.15K | -76.804878 |
| Nuclear repulsion energy | 23.760577 |
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 mPW1PW91/3-21G
| 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 |
3166 |
3022 |
48.61 |
|
|
|
| 2 |
A1 |
1701 |
1624 |
81.65 |
|
|
|
| 3 |
A1 |
1290 |
1232 |
32.36 |
|
|
|
| 4 |
B1 |
835 |
797 |
150.08 |
|
|
|
| 5 |
B2 |
3238 |
3091 |
24.21 |
|
|
|
| 6 |
B2 |
493 |
470 |
0.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5361.6 cm
-1
Scaled (by 0.9546) Zero Point Vibrational Energy (zpe) 5118.2 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 mPW1PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.479 |
| C2 |
0.000 |
0.000 |
0.826 |
| H3 |
0.000 |
0.931 |
-1.042 |
| H4 |
0.000 |
-0.931 |
-1.042 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3048 | 1.0884 | 1.0884 |
C2 | 1.3048 | | 2.0875 | 2.0875 | H3 | 1.0884 | 2.0875 | | 1.8625 | H4 | 1.0884 | 2.0875 | 1.8625 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
121.176 |
|
C2 |
C1 |
H4 |
121.176 |
| H3 |
C1 |
H4 |
117.648 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.645 |
|
|
|
| 2 |
C |
0.057 |
|
|
|
| 3 |
H |
0.294 |
|
|
|
| 4 |
H |
0.294 |
|
|
|
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 |
-2.319 |
2.319 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.011 |
0.000 |
0.000 |
| y |
0.000 |
-10.003 |
0.000 |
| z |
0.000 |
0.000 |
-13.858 |
|
| Traceless |
| | x | y | z |
| x |
-2.080 |
0.000 |
0.000 |
| y |
0.000 |
3.931 |
0.000 |
| z |
0.000 |
0.000 |
-1.851 |
|
| Polar |
| 3z2-r2 | -3.702 |
| x2-y2 | -4.007 |
| 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 |
1.173 |
0.000 |
0.000 |
| y |
0.000 |
2.321 |
0.000 |
| z |
0.000 |
0.000 |
3.595 |
<r2> (average value of r
2) Å
2
| <r2> |
17.261 |
| (<r2>)1/2 |
4.155 |
Jump to
S1C1
Energy calculated at mPW1PW91/3-21G
| | hartrees |
| Energy at 0K | -76.745206 |
| Energy at 298.15K | -76.745314 |
| HF Energy | -76.745206 |
| Nuclear repulsion energy | 23.579259 |
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 mPW1PW91/3-21G
| 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 |
3079 |
2939 |
1.36 |
|
|
|
| 2 |
A1 |
1599 |
1526 |
2.18 |
|
|
|
| 3 |
A1 |
1467 |
1400 |
4.59 |
|
|
|
| 4 |
B1 |
876 |
836 |
40.00 |
|
|
|
| 5 |
B2 |
3148 |
3005 |
6.17 |
|
|
|
| 6 |
B2 |
1051 |
1004 |
7.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5609.4 cm
-1
Scaled (by 0.9546) Zero Point Vibrational Energy (zpe) 5354.8 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 mPW1PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.483 |
| C2 |
0.000 |
0.000 |
0.834 |
| H3 |
0.000 |
0.930 |
-1.055 |
| H4 |
0.000 |
-0.930 |
-1.055 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3173 | 1.0917 | 1.0917 |
C2 | 1.3173 | | 2.1057 | 2.1057 | H3 | 1.0917 | 2.1057 | | 1.8597 | H4 | 1.0917 | 2.1057 | 1.8597 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.500 |
|
|
|
| 2 |
C |
0.019 |
|
|
|
| 3 |
H |
0.241 |
|
|
|
| 4 |
H |
0.241 |
|
|
|
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 |
-0.560 |
0.560 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.729 |
0.000 |
0.000 |
| y |
0.000 |
-11.810 |
0.000 |
| z |
0.000 |
0.000 |
-10.961 |
|
| Traceless |
| | x | y | z |
| x |
-2.343 |
0.000 |
0.000 |
| y |
0.000 |
0.534 |
0.000 |
| z |
0.000 |
0.000 |
1.809 |
|
| Polar |
| 3z2-r2 | 3.617 |
| x2-y2 | -1.918 |
| 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 |
1.186 |
0.000 |
0.000 |
| y |
0.000 |
1.884 |
0.000 |
| z |
0.000 |
0.000 |
3.653 |
<r2> (average value of r
2) Å
2
| <r2> |
17.130 |
| (<r2>)1/2 |
4.139 |