Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -79.750773 |
| Energy at 298.15K | -79.756710 |
| HF Energy | -79.750773 |
| Nuclear repulsion energy | 42.236581 |
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 B1B95/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3073 |
2931 |
0.00 |
221.04 |
0.01 |
0.02 |
| 2 |
A1g |
1468 |
1400 |
0.00 |
8.81 |
0.72 |
0.84 |
| 3 |
A1g |
1041 |
992 |
0.00 |
9.30 |
0.29 |
0.45 |
| 4 |
A1u |
306 |
292 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3071 |
2929 |
59.79 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1466 |
1398 |
6.49 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3140 |
2995 |
0.00 |
134.47 |
0.75 |
0.86 |
| 7 |
Eg |
3140 |
2995 |
0.00 |
134.47 |
0.75 |
0.86 |
| 8 |
Eg |
1552 |
1480 |
0.00 |
45.77 |
0.75 |
0.86 |
| 8 |
Eg |
1552 |
1480 |
0.00 |
45.77 |
0.75 |
0.86 |
| 9 |
Eg |
1255 |
1197 |
0.00 |
4.00 |
0.75 |
0.86 |
| 9 |
Eg |
1255 |
1197 |
0.00 |
4.00 |
0.75 |
0.86 |
| 10 |
Eu |
3167 |
3021 |
70.69 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3167 |
3021 |
70.69 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1555 |
1483 |
13.83 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1555 |
1483 |
13.83 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
858 |
819 |
8.33 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
858 |
819 |
8.33 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16740.4 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 15965.3 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 B1B95/6-31G
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 |
1.019 |
1.160 |
| H4 |
-0.882 |
-0.509 |
1.160 |
| H5 |
0.882 |
-0.509 |
1.160 |
| H6 |
0.000 |
-1.019 |
-1.160 |
| H7 |
-0.882 |
0.509 |
-1.160 |
| H8 |
0.882 |
0.509 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5256 | 1.0932 | 1.0932 | 1.0932 | 2.1758 | 2.1758 | 2.1758 |
C2 | 1.5256 | | 2.1758 | 2.1758 | 2.1758 | 1.0932 | 1.0932 | 1.0932 | H3 | 1.0932 | 2.1758 | | 1.7642 | 1.7642 | 3.0872 | 2.5334 | 2.5334 | H4 | 1.0932 | 2.1758 | 1.7642 | | 1.7642 | 2.5334 | 2.5334 | 3.0872 | H5 | 1.0932 | 2.1758 | 1.7642 | 1.7642 | | 2.5334 | 3.0872 | 2.5334 | H6 | 2.1758 | 1.0932 | 3.0872 | 2.5334 | 2.5334 | | 1.7642 | 1.7642 | H7 | 2.1758 | 1.0932 | 2.5334 | 2.5334 | 3.0872 | 1.7642 | | 1.7642 | H8 | 2.1758 | 1.0932 | 2.5334 | 3.0872 | 2.5334 | 1.7642 | 1.7642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.297 |
|
C1 |
C2 |
H7 |
111.297 |
| C1 |
C2 |
H8 |
111.297 |
|
C2 |
C1 |
H3 |
111.297 |
| C2 |
C1 |
H4 |
111.297 |
|
C2 |
C1 |
H5 |
111.297 |
| H3 |
C1 |
H4 |
107.586 |
|
H3 |
C1 |
H5 |
107.586 |
| H4 |
C1 |
H5 |
107.586 |
|
H6 |
C2 |
H7 |
107.586 |
| H6 |
C2 |
H8 |
107.586 |
|
H7 |
C2 |
H8 |
107.586 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.464 |
|
|
|
| 2 |
C |
-0.464 |
|
|
|
| 3 |
H |
0.155 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
| 5 |
H |
0.155 |
|
|
|
| 6 |
H |
0.155 |
|
|
|
| 7 |
H |
0.155 |
|
|
|
| 8 |
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.697 |
0.000 |
0.000 |
| y |
0.000 |
-14.697 |
0.000 |
| z |
0.000 |
0.000 |
-15.098 |
|
| Traceless |
| | x | y | z |
| x |
0.200 |
0.000 |
0.000 |
| y |
0.000 |
0.200 |
0.000 |
| z |
0.000 |
0.000 |
-0.401 |
|
| Polar |
| 3z2-r2 | -0.801 |
| 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 |
3.279 |
0.000 |
0.000 |
| y |
0.000 |
3.279 |
0.000 |
| z |
0.000 |
0.000 |
3.453 |
<r2> (average value of r
2) Å
2
| <r2> |
30.541 |
| (<r2>)1/2 |
5.526 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -79.746494 |
| Energy at 298.15K | |
| HF Energy | -79.746494 |
| Nuclear repulsion energy | 42.093731 |
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 B1B95/6-31G
| 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' |
3088 |
2945 |
0.00 |
|
|
|
| 2 |
A1' |
1492 |
1423 |
0.00 |
|
|
|
| 3 |
A1' |
1035 |
987 |
0.00 |
|
|
|
| 4 |
A1" |
298i |
284i |
0.00 |
|
|
|
| 5 |
A2" |
3078 |
2936 |
63.24 |
|
|
|
| 6 |
A2" |
1464 |
1397 |
6.78 |
|
|
|
| 7 |
E' |
3172 |
3026 |
58.70 |
|
|
|
| 7 |
E' |
3172 |
3026 |
58.70 |
|
|
|
| 8 |
E' |
1563 |
1490 |
15.73 |
|
|
|
| 8 |
E' |
1563 |
1490 |
15.73 |
|
|
|
| 9 |
E' |
937 |
894 |
8.52 |
|
|
|
| 9 |
E' |
937 |
894 |
8.52 |
|
|
|
| 10 |
E" |
3150 |
3004 |
0.00 |
|
|
|
| 10 |
E" |
3150 |
3004 |
0.00 |
|
|
|
| 11 |
E" |
1551 |
1479 |
0.00 |
|
|
|
| 11 |
E" |
1551 |
1479 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1154 |
0.00 |
|
|
|
| 12 |
E" |
1210 |
1154 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16513.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 15749.3 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 B1B95/6-31G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.769 |
| C2 |
0.000 |
0.000 |
-0.769 |
| H3 |
0.000 |
1.014 |
1.173 |
| H4 |
-0.879 |
-0.507 |
1.173 |
| H5 |
0.879 |
-0.507 |
1.173 |
| H6 |
0.000 |
1.014 |
-1.173 |
| H7 |
0.879 |
-0.507 |
-1.173 |
| H8 |
-0.879 |
-0.507 |
-1.173 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5373 | 1.0923 | 1.0923 | 1.0923 | 2.1911 | 2.1911 | 2.1911 |
C2 | 1.5373 | | 2.1911 | 2.1911 | 2.1911 | 1.0923 | 1.0923 | 1.0923 | H3 | 1.0923 | 2.1911 | | 1.7571 | 1.7571 | 2.3470 | 2.9319 | 2.9319 | H4 | 1.0923 | 2.1911 | 1.7571 | | 1.7571 | 2.9319 | 2.9319 | 2.3470 | H5 | 1.0923 | 2.1911 | 1.7571 | 1.7571 | | 2.9319 | 2.3470 | 2.9319 | H6 | 2.1911 | 1.0923 | 2.3470 | 2.9319 | 2.9319 | | 1.7571 | 1.7571 | H7 | 2.1911 | 1.0923 | 2.9319 | 2.9319 | 2.3470 | 1.7571 | | 1.7571 | H8 | 2.1911 | 1.0923 | 2.9319 | 2.3470 | 2.9319 | 1.7571 | 1.7571 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.754 |
|
C1 |
C2 |
H7 |
111.755 |
| C1 |
C2 |
H8 |
111.755 |
|
C2 |
C1 |
H3 |
111.754 |
| C2 |
C1 |
H4 |
111.755 |
|
C2 |
C1 |
H5 |
111.755 |
| H3 |
C1 |
H4 |
107.095 |
|
H3 |
C1 |
H5 |
107.095 |
| H4 |
C1 |
H5 |
107.095 |
|
H6 |
C2 |
H7 |
107.095 |
| H6 |
C2 |
H8 |
107.095 |
|
H7 |
C2 |
H8 |
107.095 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.473 |
|
|
|
| 2 |
C |
-0.473 |
|
|
|
| 3 |
H |
0.158 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
| 5 |
H |
0.158 |
|
|
|
| 6 |
H |
0.158 |
|
|
|
| 7 |
H |
0.158 |
|
|
|
| 8 |
H |
0.158 |
|
|
|
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 |
-14.677 |
0.000 |
0.000 |
| y |
0.000 |
-14.677 |
0.000 |
| z |
0.000 |
0.000 |
-15.020 |
|
| Traceless |
| | x | y | z |
| x |
0.171 |
0.000 |
0.000 |
| y |
0.000 |
0.171 |
0.000 |
| z |
0.000 |
0.000 |
-0.342 |
|
| Polar |
| 3z2-r2 | -0.685 |
| 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 |
3.203 |
0.000 |
0.000 |
| y |
0.000 |
3.203 |
0.000 |
| z |
0.000 |
0.000 |
3.365 |
<r2> (average value of r
2) Å
2
| <r2> |
30.766 |
| (<r2>)1/2 |
5.547 |