Jump to
S1C2
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -79.811468 |
| Energy at 298.15K | -79.817370 |
| HF Energy | -79.811468 |
| Nuclear repulsion energy | 42.173766 |
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 B3PW91/6-31+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 |
A1g |
3048 |
2927 |
0.00 |
|
|
|
| 2 |
A1g |
1428 |
1371 |
0.00 |
|
|
|
| 3 |
A1g |
1016 |
976 |
0.00 |
|
|
|
| 4 |
A1u |
310 |
297 |
0.00 |
|
|
|
| 5 |
A2u |
3047 |
2926 |
65.95 |
|
|
|
| 6 |
A2u |
1401 |
1345 |
2.48 |
|
|
|
| 7 |
Eg |
3111 |
2987 |
0.00 |
|
|
|
| 7 |
Eg |
3111 |
2987 |
0.00 |
|
|
|
| 8 |
Eg |
1505 |
1445 |
0.00 |
|
|
|
| 8 |
Eg |
1505 |
1445 |
0.00 |
|
|
|
| 9 |
Eg |
1214 |
1166 |
0.00 |
|
|
|
| 9 |
Eg |
1214 |
1166 |
0.00 |
|
|
|
| 10 |
Eu |
3134 |
3009 |
64.55 |
|
|
|
| 10 |
Eu |
3134 |
3009 |
64.56 |
|
|
|
| 11 |
Eu |
1505 |
1445 |
12.84 |
|
|
|
| 11 |
Eu |
1505 |
1445 |
12.84 |
|
|
|
| 12 |
Eu |
824 |
791 |
5.23 |
|
|
|
| 12 |
Eu |
824 |
791 |
5.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16417.0 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 15761.9 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 B3PW91/6-31+G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.020 |
1.163 |
| H4 |
-0.883 |
-0.510 |
1.163 |
| H5 |
0.883 |
-0.510 |
1.163 |
| H6 |
0.000 |
-1.020 |
-1.163 |
| H7 |
-0.883 |
0.510 |
-1.163 |
| H8 |
0.883 |
0.510 |
-1.163 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5265 | 1.0953 | 1.0953 | 1.0953 | 2.1795 | 2.1795 | 2.1795 |
C2 | 1.5265 | | 2.1795 | 2.1795 | 2.1795 | 1.0953 | 1.0953 | 1.0953 | H3 | 1.0953 | 2.1795 | | 1.7664 | 1.7664 | 3.0934 | 2.5395 | 2.5395 | H4 | 1.0953 | 2.1795 | 1.7664 | | 1.7664 | 2.5395 | 2.5395 | 3.0934 | H5 | 1.0953 | 2.1795 | 1.7664 | 1.7664 | | 2.5395 | 3.0934 | 2.5395 | H6 | 2.1795 | 1.0953 | 3.0934 | 2.5395 | 2.5395 | | 1.7664 | 1.7664 | H7 | 2.1795 | 1.0953 | 2.5395 | 2.5395 | 3.0934 | 1.7664 | | 1.7664 | H8 | 2.1795 | 1.0953 | 2.5395 | 3.0934 | 2.5395 | 1.7664 | 1.7664 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.398 |
|
C1 |
C2 |
H7 |
111.398 |
| C1 |
C2 |
H8 |
111.398 |
|
C2 |
C1 |
H3 |
111.398 |
| C2 |
C1 |
H4 |
111.398 |
|
C2 |
C1 |
H5 |
111.398 |
| H3 |
C1 |
H4 |
107.478 |
|
H3 |
C1 |
H5 |
107.478 |
| H4 |
C1 |
H5 |
107.478 |
|
H6 |
C2 |
H7 |
107.478 |
| H6 |
C2 |
H8 |
107.478 |
|
H7 |
C2 |
H8 |
107.478 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.482 |
|
|
|
| 2 |
C |
-0.482 |
|
|
|
| 3 |
H |
0.161 |
|
|
|
| 4 |
H |
0.161 |
|
|
|
| 5 |
H |
0.161 |
|
|
|
| 6 |
H |
0.161 |
|
|
|
| 7 |
H |
0.161 |
|
|
|
| 8 |
H |
0.161 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.875 |
0.000 |
0.000 |
| y |
0.000 |
-14.875 |
0.000 |
| z |
0.000 |
0.000 |
-15.514 |
|
| Traceless |
| | x | y | z |
| x |
0.320 |
0.000 |
0.000 |
| y |
0.000 |
0.320 |
0.000 |
| z |
0.000 |
0.000 |
-0.639 |
|
| Polar |
| 3z2-r2 | -1.278 |
| x2-y2 | 0.000 |
| 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 |
3.615 |
0.000 |
0.000 |
| y |
0.000 |
3.615 |
0.000 |
| z |
0.000 |
0.000 |
3.997 |
<r2> (average value of r
2) Å
2
| <r2> |
30.769 |
| (<r2>)1/2 |
5.547 |
Jump to
S1C1
Energy calculated at B3PW91/6-31+G**
| | hartrees |
| Energy at 0K | -79.807105 |
| Energy at 298.15K | |
| HF Energy | -79.807105 |
| Nuclear repulsion energy | 42.015260 |
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 B3PW91/6-31+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' |
3063 |
2941 |
0.00 |
|
|
|
| 2 |
A1' |
1448 |
1391 |
0.00 |
|
|
|
| 3 |
A1' |
1014 |
973 |
0.00 |
|
|
|
| 4 |
A1" |
301i |
289i |
0.00 |
|
|
|
| 5 |
A2" |
3055 |
2933 |
69.87 |
|
|
|
| 6 |
A2" |
1401 |
1345 |
2.37 |
|
|
|
| 7 |
E' |
3141 |
3015 |
53.31 |
|
|
|
| 7 |
E' |
3141 |
3015 |
53.31 |
|
|
|
| 8 |
E' |
1511 |
1451 |
15.02 |
|
|
|
| 8 |
E' |
1511 |
1451 |
15.02 |
|
|
|
| 9 |
E' |
901 |
865 |
4.72 |
|
|
|
| 9 |
E' |
901 |
865 |
4.72 |
|
|
|
| 10 |
E" |
3120 |
2996 |
0.00 |
|
|
|
| 10 |
E" |
3120 |
2996 |
0.00 |
|
|
|
| 11 |
E" |
1502 |
1442 |
0.00 |
|
|
|
| 11 |
E" |
1502 |
1442 |
0.00 |
|
|
|
| 12 |
E" |
1166 |
1119 |
0.00 |
|
|
|
| 12 |
E" |
1166 |
1119 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16180.1 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 15534.6 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 B3PW91/6-31+G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.770 |
| C2 |
0.000 |
0.000 |
-0.770 |
| H3 |
0.000 |
1.015 |
1.178 |
| H4 |
-0.879 |
-0.508 |
1.178 |
| H5 |
0.879 |
-0.508 |
1.178 |
| H6 |
0.000 |
1.015 |
-1.178 |
| H7 |
0.879 |
-0.508 |
-1.178 |
| H8 |
-0.879 |
-0.508 |
-1.178 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5396 | 1.0943 | 1.0943 | 1.0943 | 2.1963 | 2.1963 | 2.1963 |
C2 | 1.5396 | | 2.1963 | 2.1963 | 2.1963 | 1.0943 | 1.0943 | 1.0943 | H3 | 1.0943 | 2.1963 | | 1.7589 | 1.7589 | 2.3553 | 2.9396 | 2.9396 | H4 | 1.0943 | 2.1963 | 1.7589 | | 1.7589 | 2.9396 | 2.9396 | 2.3553 | H5 | 1.0943 | 2.1963 | 1.7589 | 1.7589 | | 2.9396 | 2.3553 | 2.9396 | H6 | 2.1963 | 1.0943 | 2.3553 | 2.9396 | 2.9396 | | 1.7589 | 1.7589 | H7 | 2.1963 | 1.0943 | 2.9396 | 2.9396 | 2.3553 | 1.7589 | | 1.7589 | H8 | 2.1963 | 1.0943 | 2.9396 | 2.3553 | 2.9396 | 1.7589 | 1.7589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.883 |
|
C1 |
C2 |
H7 |
111.883 |
| C1 |
C2 |
H8 |
111.883 |
|
C2 |
C1 |
H3 |
111.883 |
| C2 |
C1 |
H4 |
111.883 |
|
C2 |
C1 |
H5 |
111.883 |
| H3 |
C1 |
H4 |
106.956 |
|
H3 |
C1 |
H5 |
106.956 |
| H4 |
C1 |
H5 |
106.956 |
|
H6 |
C2 |
H7 |
106.956 |
| H6 |
C2 |
H8 |
106.956 |
|
H7 |
C2 |
H8 |
106.956 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.491 |
|
|
|
| 2 |
C |
-0.491 |
|
|
|
| 3 |
H |
0.164 |
|
|
|
| 4 |
H |
0.164 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
| 6 |
H |
0.164 |
|
|
|
| 7 |
H |
0.164 |
|
|
|
| 8 |
H |
0.164 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.869 |
0.000 |
0.000 |
| y |
0.000 |
-14.869 |
0.000 |
| z |
0.000 |
0.000 |
-15.480 |
|
| Traceless |
| | x | y | z |
| x |
0.306 |
0.000 |
0.000 |
| y |
0.000 |
0.306 |
0.000 |
| z |
0.000 |
0.000 |
-0.611 |
|
| Polar |
| 3z2-r2 | -1.223 |
| x2-y2 | 0.000 |
| 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 |
3.564 |
0.000 |
0.000 |
| y |
0.000 |
3.564 |
0.000 |
| z |
0.000 |
0.000 |
3.901 |
<r2> (average value of r
2) Å
2
| <r2> |
31.034 |
| (<r2>)1/2 |
5.571 |