Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -79.825054 |
| Energy at 298.15K | -79.830962 |
| HF Energy | -79.825054 |
| Nuclear repulsion energy | 42.227014 |
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 B3PW91/6-311G**
| 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 |
3036 |
2924 |
0.00 |
259.55 |
0.01 |
0.01 |
| 2 |
A1g |
1421 |
1368 |
0.00 |
2.97 |
0.74 |
0.85 |
| 3 |
A1g |
1015 |
977 |
0.00 |
9.52 |
0.27 |
0.42 |
| 4 |
A1u |
310 |
298 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3036 |
2924 |
61.29 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1399 |
1347 |
2.44 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3092 |
2977 |
0.00 |
145.73 |
0.75 |
0.86 |
| 7 |
Eg |
3092 |
2977 |
0.00 |
145.72 |
0.75 |
0.86 |
| 8 |
Eg |
1499 |
1444 |
0.00 |
24.64 |
0.75 |
0.86 |
| 8 |
Eg |
1499 |
1444 |
0.00 |
24.64 |
0.75 |
0.86 |
| 9 |
Eg |
1213 |
1168 |
0.00 |
0.66 |
0.75 |
0.86 |
| 9 |
Eg |
1213 |
1168 |
0.00 |
0.66 |
0.75 |
0.86 |
| 10 |
Eu |
3116 |
3001 |
68.08 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3116 |
3001 |
68.08 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1500 |
1445 |
11.46 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1500 |
1445 |
11.46 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
794 |
5.46 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
794 |
5.46 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16352.7 cm
-1
Scaled (by 0.9631) 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 B3PW91/6-311G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.762 |
| C2 |
0.000 |
0.000 |
-0.762 |
| H3 |
0.000 |
1.018 |
1.162 |
| H4 |
-0.882 |
-0.509 |
1.162 |
| H5 |
0.882 |
-0.509 |
1.162 |
| H6 |
0.000 |
-1.018 |
-1.162 |
| H7 |
-0.882 |
0.509 |
-1.162 |
| H8 |
0.882 |
0.509 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5245 | 1.0939 | 1.0939 | 1.0939 | 2.1769 | 2.1769 | 2.1769 |
C2 | 1.5245 | | 2.1769 | 2.1769 | 2.1769 | 1.0939 | 1.0939 | 1.0939 | H3 | 1.0939 | 2.1769 | | 1.7639 | 1.7639 | 3.0898 | 2.5369 | 2.5369 | H4 | 1.0939 | 2.1769 | 1.7639 | | 1.7639 | 2.5369 | 2.5369 | 3.0898 | H5 | 1.0939 | 2.1769 | 1.7639 | 1.7639 | | 2.5369 | 3.0898 | 2.5369 | H6 | 2.1769 | 1.0939 | 3.0898 | 2.5369 | 2.5369 | | 1.7639 | 1.7639 | H7 | 2.1769 | 1.0939 | 2.5369 | 2.5369 | 3.0898 | 1.7639 | | 1.7639 | H8 | 2.1769 | 1.0939 | 2.5369 | 3.0898 | 2.5369 | 1.7639 | 1.7639 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.419 |
|
C1 |
C2 |
H7 |
111.419 |
| C1 |
C2 |
H8 |
111.419 |
|
C2 |
C1 |
H3 |
111.419 |
| C2 |
C1 |
H4 |
111.419 |
|
C2 |
C1 |
H5 |
111.419 |
| H3 |
C1 |
H4 |
107.456 |
|
H3 |
C1 |
H5 |
107.456 |
| H4 |
C1 |
H5 |
107.456 |
|
H6 |
C2 |
H7 |
107.456 |
| H6 |
C2 |
H8 |
107.456 |
|
H7 |
C2 |
H8 |
107.456 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.359 |
|
|
|
| 2 |
C |
-0.359 |
|
|
|
| 3 |
H |
0.120 |
|
|
|
| 4 |
H |
0.120 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.120 |
|
|
|
| 7 |
H |
0.120 |
|
|
|
| 8 |
H |
0.120 |
|
|
|
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 |
-14.819 |
0.000 |
0.000 |
| y |
0.000 |
-14.819 |
0.000 |
| z |
0.000 |
0.000 |
-15.431 |
|
| 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 | -1.222 |
| 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 |
3.609 |
0.000 |
0.000 |
| y |
0.000 |
3.609 |
0.000 |
| z |
0.000 |
0.000 |
4.000 |
<r2> (average value of r
2) Å
2
| <r2> |
30.676 |
| (<r2>)1/2 |
5.539 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -79.820690 |
| Energy at 298.15K | |
| HF Energy | -79.820690 |
| Nuclear repulsion energy | 42.070784 |
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 B3PW91/6-311G**
| 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' |
3051 |
2939 |
0.00 |
|
|
|
| 2 |
A1' |
1436 |
1383 |
0.00 |
|
|
|
| 3 |
A1' |
1012 |
975 |
0.00 |
|
|
|
| 4 |
A1" |
302i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3044 |
2932 |
63.85 |
|
|
|
| 6 |
A2" |
1397 |
1345 |
2.46 |
|
|
|
| 7 |
E' |
3123 |
3008 |
56.39 |
|
|
|
| 7 |
E' |
3123 |
3008 |
56.39 |
|
|
|
| 8 |
E' |
1506 |
1450 |
13.57 |
|
|
|
| 8 |
E' |
1506 |
1450 |
13.57 |
|
|
|
| 9 |
E' |
895 |
862 |
4.97 |
|
|
|
| 9 |
E' |
895 |
862 |
4.97 |
|
|
|
| 10 |
E" |
3102 |
2987 |
0.00 |
|
|
|
| 10 |
E" |
3102 |
2987 |
0.00 |
|
|
|
| 11 |
E" |
1497 |
1442 |
0.00 |
|
|
|
| 11 |
E" |
1497 |
1442 |
0.00 |
|
|
|
| 12 |
E" |
1164 |
1121 |
0.00 |
|
|
|
| 12 |
E" |
1164 |
1121 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16105.4 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 15511.1 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 B3PW91/6-311G**
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 |
1.176 |
| H4 |
-0.878 |
-0.507 |
1.176 |
| H5 |
0.878 |
-0.507 |
1.176 |
| H6 |
0.000 |
1.014 |
-1.176 |
| H7 |
0.878 |
-0.507 |
-1.176 |
| H8 |
-0.878 |
-0.507 |
-1.176 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5377 | 1.0928 | 1.0928 | 1.0928 | 2.1934 | 2.1934 | 2.1934 |
C2 | 1.5377 | | 2.1934 | 2.1934 | 2.1934 | 1.0928 | 1.0928 | 1.0928 | H3 | 1.0928 | 2.1934 | | 1.7565 | 1.7565 | 2.3521 | 2.9356 | 2.9356 | H4 | 1.0928 | 2.1934 | 1.7565 | | 1.7565 | 2.9356 | 2.9356 | 2.3521 | H5 | 1.0928 | 2.1934 | 1.7565 | 1.7565 | | 2.9356 | 2.3521 | 2.9356 | H6 | 2.1934 | 1.0928 | 2.3521 | 2.9356 | 2.9356 | | 1.7565 | 1.7565 | H7 | 2.1934 | 1.0928 | 2.9356 | 2.9356 | 2.3521 | 1.7565 | | 1.7565 | H8 | 2.1934 | 1.0928 | 2.9356 | 2.3521 | 2.9356 | 1.7565 | 1.7565 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.877 |
|
C1 |
C2 |
H7 |
111.877 |
| C1 |
C2 |
H8 |
111.877 |
|
C2 |
C1 |
H3 |
111.877 |
| C2 |
C1 |
H4 |
111.877 |
|
C2 |
C1 |
H5 |
111.877 |
| H3 |
C1 |
H4 |
106.962 |
|
H3 |
C1 |
H5 |
106.962 |
| H4 |
C1 |
H5 |
106.962 |
|
H6 |
C2 |
H7 |
106.962 |
| H6 |
C2 |
H8 |
106.962 |
|
H7 |
C2 |
H8 |
106.962 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.371 |
|
|
|
| 2 |
C |
-0.371 |
|
|
|
| 3 |
H |
0.124 |
|
|
|
| 4 |
H |
0.124 |
|
|
|
| 5 |
H |
0.124 |
|
|
|
| 6 |
H |
0.124 |
|
|
|
| 7 |
H |
0.124 |
|
|
|
| 8 |
H |
0.124 |
|
|
|
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 |
-14.811 |
0.000 |
0.000 |
| y |
0.000 |
-14.811 |
0.000 |
| z |
0.000 |
0.000 |
-15.410 |
|
| Traceless |
| | x | y | z |
| x |
0.299 |
0.000 |
0.000 |
| y |
0.000 |
0.299 |
0.000 |
| z |
0.000 |
0.000 |
-0.599 |
|
| Polar |
| 3z2-r2 | -1.197 |
| 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 |
3.545 |
0.000 |
0.000 |
| y |
0.000 |
3.545 |
0.000 |
| z |
0.000 |
0.000 |
3.917 |
<r2> (average value of r
2) Å
2
| <r2> |
30.938 |
| (<r2>)1/2 |
5.562 |