Jump to
S2C1
Energy calculated at B3LYP/aug-cc-pVQZ
| hartrees |
Energy at 0K | -77.300451 |
Energy at 298.15K | -77.300155 |
Nuclear repulsion energy | 23.975431 |
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 B3LYP/aug-cc-pVQZ
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 |
3113 |
3016 |
48.50 |
|
|
|
2 |
A1 |
1712 |
1659 |
90.03 |
|
|
|
3 |
A1 |
1217 |
1179 |
24.11 |
|
|
|
4 |
B1 |
759 |
735 |
76.35 |
|
|
|
5 |
B2 |
3190 |
3090 |
19.54 |
|
|
|
6 |
B2 |
349 |
338 |
8.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5169.7 cm
-1
Scaled (by 0.9689) Zero Point Vibrational Energy (zpe) 5009.0 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 B3LYP/aug-cc-pVQZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-0.474 |
C2 |
0.000 |
0.000 |
0.816 |
H3 |
0.000 |
0.937 |
-1.024 |
H4 |
0.000 |
-0.937 |
-1.024 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
H4 |
C1 | | 1.2898 | 1.0861 | 1.0861 |
C2 | 1.2898 | | 2.0644 | 2.0644 | H3 | 1.0861 | 2.0644 | | 1.8732 | H4 | 1.0861 | 2.0644 | 1.8732 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C2 |
C1 |
H3 |
120.420 |
|
C2 |
C1 |
H4 |
120.420 |
H3 |
C1 |
H4 |
119.161 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.702 |
|
|
|
2 |
C |
-0.127 |
|
|
|
3 |
H |
0.415 |
|
|
|
4 |
H |
0.415 |
|
|
|
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 |
-2.514 |
2.514 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.422 |
0.000 |
0.000 |
y |
0.000 |
-10.622 |
0.000 |
z |
0.000 |
0.000 |
-14.446 |
|
Traceless |
| x | y | z |
x |
-1.888 |
0.000 |
0.000 |
y |
0.000 |
3.812 |
0.000 |
z |
0.000 |
0.000 |
-1.924 |
|
Polar |
3z2-r2 | -3.848 |
x2-y2 | -3.800 |
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 |
3.107 |
0.000 |
0.000 |
y |
0.000 |
3.345 |
0.000 |
z |
0.000 |
0.000 |
4.528 |
<r2> (average value of r
2) Å
2
<r2> |
17.414 |
(<r2>)1/2 |
4.173 |
Jump to
S1C1
Energy calculated at B3LYP/aug-cc-pVQZ
| hartrees |
Energy at 0K | -77.224591 |
Energy at 298.15K | -77.224649 |
HF Energy | -77.224591 |
Nuclear repulsion energy | 23.706674 |
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 B3LYP/aug-cc-pVQZ
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 |
3019 |
2925 |
5.63 |
|
|
|
2 |
A1 |
1582 |
1533 |
5.32 |
|
|
|
3 |
A1 |
1399 |
1356 |
2.25 |
|
|
|
4 |
B1 |
757 |
734 |
0.40 |
|
|
|
5 |
B2 |
3086 |
2990 |
3.23 |
|
|
|
6 |
B2 |
992 |
962 |
2.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5417.6 cm
-1
Scaled (by 0.9689) Zero Point Vibrational Energy (zpe) 5249.1 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 B3LYP/aug-cc-pVQZ
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 |
-1.045 |
H4 |
0.000 |
-0.932 |
-1.045 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
H3 |
H4 |
C1 | | 1.3082 | 1.0900 | 1.0900 |
C2 | 1.3082 | | 2.0923 | 2.0923 | H3 | 1.0900 | 2.0923 | | 1.8645 | H4 | 1.0900 | 2.0923 | 1.8645 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/aug-cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.723 |
|
|
|
2 |
C |
-0.046 |
|
|
|
3 |
H |
0.384 |
|
|
|
4 |
H |
0.384 |
|
|
|
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 |
-0.658 |
0.658 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-14.054 |
0.000 |
0.000 |
y |
0.000 |
-12.260 |
0.000 |
z |
0.000 |
0.000 |
-11.512 |
|
Traceless |
| x | y | z |
x |
-2.168 |
0.000 |
0.000 |
y |
0.000 |
0.523 |
0.000 |
z |
0.000 |
0.000 |
1.646 |
|
Polar |
3z2-r2 | 3.292 |
x2-y2 | -1.794 |
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 |
3.773 |
0.000 |
0.000 |
y |
0.000 |
3.361 |
0.000 |
z |
0.000 |
0.000 |
4.775 |
<r2> (average value of r
2) Å
2
<r2> |
17.295 |
(<r2>)1/2 |
4.159 |