Jump to
S1C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -79.830485 |
| Energy at 298.15K | -79.836401 |
| HF Energy | -79.830485 |
| Nuclear repulsion energy | 42.288591 |
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 mPW1PW91/6-311G**
| 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 |
3053 |
2921 |
0.00 |
257.70 |
0.01 |
0.01 |
| 2 |
A1g |
1429 |
1367 |
0.00 |
2.83 |
0.74 |
0.85 |
| 3 |
A1g |
1024 |
979 |
0.00 |
9.70 |
0.26 |
0.42 |
| 4 |
A1u |
312 |
298 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3053 |
2921 |
60.41 |
0.00 |
0.01 |
0.00 |
| 6 |
A2u |
1405 |
1344 |
2.54 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3110 |
2976 |
0.00 |
143.65 |
0.75 |
0.86 |
| 7 |
Eg |
3110 |
2976 |
0.00 |
143.66 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1442 |
0.00 |
24.40 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1442 |
0.00 |
24.40 |
0.75 |
0.86 |
| 9 |
Eg |
1220 |
1167 |
0.00 |
0.66 |
0.75 |
0.86 |
| 9 |
Eg |
1220 |
1167 |
0.00 |
0.66 |
0.75 |
0.86 |
| 10 |
Eu |
3135 |
3000 |
67.57 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3135 |
3000 |
67.57 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1507 |
1442 |
11.51 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1507 |
1442 |
11.51 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
792 |
5.34 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
792 |
5.34 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16445.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15732.9 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 mPW1PW91/6-311G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.761 |
| C2 |
0.000 |
0.000 |
-0.761 |
| H3 |
0.000 |
1.017 |
1.160 |
| H4 |
-0.881 |
-0.509 |
1.160 |
| H5 |
0.881 |
-0.509 |
1.160 |
| H6 |
0.000 |
-1.017 |
-1.160 |
| H7 |
-0.881 |
0.509 |
-1.160 |
| H8 |
0.881 |
0.509 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5221 | 1.0925 | 1.0925 | 1.0925 | 2.1735 | 2.1735 | 2.1735 |
C2 | 1.5221 | | 2.1735 | 2.1735 | 2.1735 | 1.0925 | 1.0925 | 1.0925 | H3 | 1.0925 | 2.1735 | | 1.7617 | 1.7617 | 3.0852 | 2.5328 | 2.5328 | H4 | 1.0925 | 2.1735 | 1.7617 | | 1.7617 | 2.5328 | 2.5328 | 3.0852 | H5 | 1.0925 | 2.1735 | 1.7617 | 1.7617 | | 2.5328 | 3.0852 | 2.5328 | H6 | 2.1735 | 1.0925 | 3.0852 | 2.5328 | 2.5328 | | 1.7617 | 1.7617 | H7 | 2.1735 | 1.0925 | 2.5328 | 2.5328 | 3.0852 | 1.7617 | | 1.7617 | H8 | 2.1735 | 1.0925 | 2.5328 | 3.0852 | 2.5328 | 1.7617 | 1.7617 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.407 |
|
C1 |
C2 |
H7 |
111.407 |
| C1 |
C2 |
H8 |
111.407 |
|
C2 |
C1 |
H3 |
111.407 |
| C2 |
C1 |
H4 |
111.407 |
|
C2 |
C1 |
H5 |
111.407 |
| H3 |
C1 |
H4 |
107.468 |
|
H3 |
C1 |
H5 |
107.468 |
| H4 |
C1 |
H5 |
107.468 |
|
H6 |
C2 |
H7 |
107.468 |
| H6 |
C2 |
H8 |
107.468 |
|
H7 |
C2 |
H8 |
107.468 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.360 |
|
|
|
| 2 |
C |
-0.360 |
|
|
|
| 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 |
-14.809 |
0.000 |
0.000 |
| y |
0.000 |
-14.809 |
0.000 |
| z |
0.000 |
0.000 |
-15.422 |
|
| Traceless |
| | x | y | z |
| x |
0.306 |
0.000 |
0.000 |
| y |
0.000 |
0.306 |
0.000 |
| z |
0.000 |
0.000 |
-0.613 |
|
| Polar |
| 3z2-r2 | -1.226 |
| 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 |
3.590 |
0.000 |
0.000 |
| y |
0.000 |
3.590 |
0.000 |
| z |
0.000 |
0.000 |
3.971 |
<r2> (average value of r
2) Å
2
| <r2> |
30.606 |
| (<r2>)1/2 |
5.532 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -79.826077 |
| Energy at 298.15K | |
| HF Energy | -79.826077 |
| Nuclear repulsion energy | 42.132947 |
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 mPW1PW91/6-311G**
| 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' |
3069 |
2936 |
0.00 |
|
|
|
| 2 |
A1' |
1444 |
1382 |
0.00 |
|
|
|
| 3 |
A1' |
1022 |
977 |
0.00 |
|
|
|
| 4 |
A1" |
303i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3061 |
2928 |
63.22 |
|
|
|
| 6 |
A2" |
1404 |
1343 |
2.53 |
|
|
|
| 7 |
E' |
3142 |
3006 |
56.00 |
|
|
|
| 7 |
E' |
3142 |
3006 |
56.00 |
|
|
|
| 8 |
E' |
1513 |
1448 |
13.65 |
|
|
|
| 8 |
E' |
1513 |
1448 |
13.65 |
|
|
|
| 9 |
E' |
899 |
860 |
4.85 |
|
|
|
| 9 |
E' |
899 |
860 |
4.85 |
|
|
|
| 10 |
E" |
3120 |
2985 |
0.00 |
|
|
|
| 10 |
E" |
3120 |
2985 |
0.00 |
|
|
|
| 11 |
E" |
1504 |
1439 |
0.00 |
|
|
|
| 11 |
E" |
1504 |
1439 |
0.00 |
|
|
|
| 12 |
E" |
1170 |
1120 |
0.00 |
|
|
|
| 12 |
E" |
1170 |
1120 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16197.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15496.3 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 mPW1PW91/6-311G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.768 |
| C2 |
0.000 |
0.000 |
-0.768 |
| H3 |
0.000 |
1.013 |
1.174 |
| H4 |
-0.877 |
-0.506 |
1.174 |
| H5 |
0.877 |
-0.506 |
1.174 |
| H6 |
0.000 |
1.013 |
-1.174 |
| H7 |
0.877 |
-0.506 |
-1.174 |
| H8 |
-0.877 |
-0.506 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5352 | 1.0914 | 1.0914 | 1.0914 | 2.1900 | 2.1900 | 2.1900 |
C2 | 1.5352 | | 2.1900 | 2.1900 | 2.1900 | 1.0914 | 1.0914 | 1.0914 | H3 | 1.0914 | 2.1900 | | 1.7543 | 1.7543 | 2.3482 | 2.9311 | 2.9311 | H4 | 1.0914 | 2.1900 | 1.7543 | | 1.7543 | 2.9311 | 2.9311 | 2.3482 | H5 | 1.0914 | 2.1900 | 1.7543 | 1.7543 | | 2.9311 | 2.3482 | 2.9311 | H6 | 2.1900 | 1.0914 | 2.3482 | 2.9311 | 2.9311 | | 1.7543 | 1.7543 | H7 | 2.1900 | 1.0914 | 2.9311 | 2.9311 | 2.3482 | 1.7543 | | 1.7543 | H8 | 2.1900 | 1.0914 | 2.9311 | 2.3482 | 2.9311 | 1.7543 | 1.7543 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.870 |
|
C1 |
C2 |
H7 |
111.870 |
| C1 |
C2 |
H8 |
111.870 |
|
C2 |
C1 |
H3 |
111.870 |
| C2 |
C1 |
H4 |
111.870 |
|
C2 |
C1 |
H5 |
111.870 |
| H3 |
C1 |
H4 |
106.970 |
|
H3 |
C1 |
H5 |
106.970 |
| H4 |
C1 |
H5 |
106.970 |
|
H6 |
C2 |
H7 |
106.970 |
| H6 |
C2 |
H8 |
106.970 |
|
H7 |
C2 |
H8 |
106.970 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.372 |
|
|
|
| 2 |
C |
-0.372 |
|
|
|
| 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 |
-14.800 |
0.000 |
0.000 |
| y |
0.000 |
-14.800 |
0.000 |
| z |
0.000 |
0.000 |
-15.401 |
|
| Traceless |
| | x | y | z |
| x |
0.300 |
0.000 |
0.000 |
| y |
0.000 |
0.300 |
0.000 |
| z |
0.000 |
0.000 |
-0.601 |
|
| Polar |
| 3z2-r2 | -1.201 |
| 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 |
3.527 |
0.000 |
0.000 |
| y |
0.000 |
3.527 |
0.000 |
| z |
0.000 |
0.000 |
3.889 |
<r2> (average value of r
2) Å
2
| <r2> |
30.865 |
| (<r2>)1/2 |
5.556 |