Jump to
S2C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -77.226840 |
| Energy at 298.15K | -77.226481 |
| Nuclear repulsion energy | 23.835435 |
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 B1B95/6-31+G**
| 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 |
3152 |
3015 |
50.64 |
|
|
|
| 2 |
A1 |
1729 |
1654 |
94.21 |
|
|
|
| 3 |
A1 |
1208 |
1155 |
26.53 |
|
|
|
| 4 |
B1 |
752 |
719 |
112.08 |
|
|
|
| 5 |
B2 |
3237 |
3097 |
22.78 |
|
|
|
| 6 |
B2 |
300 |
287 |
4.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5188.9 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 4963.7 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 B1B95/6-31+G**
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 |
0.821 |
| H3 |
0.000 |
0.938 |
-1.031 |
| H4 |
0.000 |
-0.938 |
-1.031 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2990 | 1.0892 | 1.0892 |
C2 | 1.2990 | | 2.0762 | 2.0762 | H3 | 1.0892 | 2.0762 | | 1.8769 | H4 | 1.0892 | 2.0762 | 1.8769 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.507 |
|
C2 |
C1 |
H4 |
120.507 |
| H3 |
C1 |
H4 |
118.987 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.070 |
|
|
|
| 2 |
C |
-0.360 |
|
|
|
| 3 |
H |
0.215 |
|
|
|
| 4 |
H |
0.215 |
|
|
|
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 |
-2.458 |
2.458 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.524 |
0.000 |
0.000 |
| y |
0.000 |
-10.413 |
0.000 |
| z |
0.000 |
0.000 |
-14.338 |
|
| Traceless |
| | x | y | z |
| x |
-2.149 |
0.000 |
0.000 |
| y |
0.000 |
4.018 |
0.000 |
| z |
0.000 |
0.000 |
-1.869 |
|
| Polar |
| 3z2-r2 | -3.738 |
| x2-y2 | -4.111 |
| 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 |
2.520 |
0.000 |
0.000 |
| y |
0.000 |
2.825 |
0.000 |
| z |
0.000 |
0.000 |
4.532 |
<r2> (average value of r
2) Å
2
| <r2> |
17.479 |
| (<r2>)1/2 |
4.181 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -77.152886 |
| Energy at 298.15K | -77.152945 |
| HF Energy | -77.152886 |
| Nuclear repulsion energy | 23.596913 |
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 B1B95/6-31+G**
| 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 |
3080 |
2946 |
3.01 |
|
|
|
| 2 |
A1 |
1607 |
1537 |
4.19 |
|
|
|
| 3 |
A1 |
1398 |
1338 |
1.40 |
|
|
|
| 4 |
B1 |
765 |
732 |
6.93 |
|
|
|
| 5 |
B2 |
3162 |
3025 |
3.11 |
|
|
|
| 6 |
B2 |
991 |
948 |
6.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5501.9 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 5263.1 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 B1B95/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.484 |
| C2 |
0.000 |
0.000 |
0.833 |
| H3 |
0.000 |
0.935 |
-1.046 |
| H4 |
0.000 |
-0.935 |
-1.046 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3166 | 1.0913 | 1.0913 |
C2 | 1.3166 | | 2.0988 | 2.0988 | H3 | 1.0913 | 2.0988 | | 1.8706 | H4 | 1.0913 | 2.0988 | 1.8706 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.299 |
|
|
|
| 2 |
C |
-0.043 |
|
|
|
| 3 |
H |
0.171 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
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 |
-0.672 |
0.672 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.106 |
0.000 |
0.000 |
| y |
0.000 |
-12.102 |
0.000 |
| z |
0.000 |
0.000 |
-11.383 |
|
| Traceless |
| | x | y | z |
| x |
-2.363 |
0.000 |
0.000 |
| y |
0.000 |
0.643 |
0.000 |
| z |
0.000 |
0.000 |
1.720 |
|
| Polar |
| 3z2-r2 | 3.441 |
| x2-y2 | -2.004 |
| 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 |
2.788 |
0.000 |
0.000 |
| y |
0.000 |
2.517 |
0.000 |
| z |
0.000 |
0.000 |
4.501 |
<r2> (average value of r
2) Å
2
| <r2> |
17.330 |
| (<r2>)1/2 |
4.163 |