Jump to
S2C1
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -77.234970 |
| Energy at 298.15K | -77.234643 |
| Nuclear repulsion energy | 23.819363 |
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 mPW1PW91/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3174 |
3020 |
42.75 |
|
|
|
| 2 |
A1 |
1736 |
1652 |
83.21 |
|
|
|
| 3 |
A1 |
1229 |
1169 |
24.85 |
|
|
|
| 4 |
B1 |
761 |
724 |
97.74 |
|
|
|
| 5 |
B2 |
3258 |
3100 |
19.42 |
|
|
|
| 6 |
B2 |
324 |
308 |
2.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5240.9 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 4986.7 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 mPW1PW91/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.478 |
| C2 |
0.000 |
0.000 |
0.822 |
| H3 |
0.000 |
0.936 |
-1.032 |
| H4 |
0.000 |
-0.936 |
-1.032 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3008 | 1.0881 | 1.0881 |
C2 | 1.3008 | | 2.0779 | 2.0779 | H3 | 1.0881 | 2.0779 | | 1.8728 | H4 | 1.0881 | 2.0779 | 1.8728 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.613 |
|
C2 |
C1 |
H4 |
120.613 |
| H3 |
C1 |
H4 |
118.774 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.416 |
|
|
|
| 2 |
C |
0.013 |
|
|
|
| 3 |
H |
0.201 |
|
|
|
| 4 |
H |
0.201 |
|
|
|
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 |
-2.294 |
2.294 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.683 |
0.000 |
0.000 |
| y |
0.000 |
-9.916 |
0.000 |
| z |
0.000 |
0.000 |
-13.689 |
|
| Traceless |
| | x | y | z |
| x |
-1.880 |
0.000 |
0.000 |
| y |
0.000 |
3.770 |
0.000 |
| z |
0.000 |
0.000 |
-1.889 |
|
| Polar |
| 3z2-r2 | -3.778 |
| x2-y2 | -3.767 |
| 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 |
1.461 |
0.000 |
0.000 |
| y |
0.000 |
2.465 |
0.000 |
| z |
0.000 |
0.000 |
3.770 |
<r2> (average value of r
2) Å
2
| <r2> |
17.081 |
| (<r2>)1/2 |
4.133 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31G**
| | hartrees |
| Energy at 0K | -77.171958 |
| Energy at 298.15K | -77.172033 |
| HF Energy | -77.171958 |
| Nuclear repulsion energy | 23.602051 |
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 mPW1PW91/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3086 |
2936 |
3.85 |
|
|
|
| 2 |
A1 |
1621 |
1542 |
3.70 |
|
|
|
| 3 |
A1 |
1415 |
1346 |
2.25 |
|
|
|
| 4 |
B1 |
805 |
766 |
16.08 |
|
|
|
| 5 |
B2 |
3164 |
3010 |
7.25 |
|
|
|
| 6 |
B2 |
1001 |
953 |
3.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5546.0 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 5277.0 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 mPW1PW91/6-31G**
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 |
0.833 |
| H3 |
0.000 |
0.933 |
-1.050 |
| H4 |
0.000 |
-0.933 |
-1.050 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3155 | 1.0920 | 1.0920 |
C2 | 1.3155 | | 2.1013 | 2.1013 | H3 | 1.0920 | 2.1013 | | 1.8662 | H4 | 1.0920 | 2.1013 | 1.8662 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.301 |
|
|
|
| 2 |
C |
-0.009 |
|
|
|
| 3 |
H |
0.155 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
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 |
-0.528 |
0.528 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.395 |
0.000 |
0.000 |
| y |
0.000 |
-11.631 |
0.000 |
| z |
0.000 |
0.000 |
-10.849 |
|
| Traceless |
| | x | y | z |
| x |
-2.155 |
0.000 |
0.000 |
| y |
0.000 |
0.491 |
0.000 |
| z |
0.000 |
0.000 |
1.664 |
|
| Polar |
| 3z2-r2 | 3.327 |
| x2-y2 | -1.764 |
| 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 |
1.565 |
0.000 |
0.000 |
| y |
0.000 |
2.137 |
0.000 |
| z |
0.000 |
0.000 |
3.884 |
<r2> (average value of r
2) Å
2
| <r2> |
16.975 |
| (<r2>)1/2 |
4.120 |