Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -79.824838 |
| Energy at 298.15K | -79.830756 |
| HF Energy | -79.824838 |
| Nuclear repulsion energy | 42.223842 |
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 wB97X-D/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 |
3047 |
2914 |
0.00 |
255.99 |
0.01 |
0.02 |
| 2 |
A1g |
1434 |
1372 |
0.00 |
2.58 |
0.69 |
0.82 |
| 3 |
A1g |
1015 |
971 |
0.00 |
10.64 |
0.27 |
0.42 |
| 4 |
A1u |
311 |
297 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3045 |
2913 |
61.60 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1408 |
1346 |
2.82 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3106 |
2971 |
0.00 |
144.49 |
0.75 |
0.86 |
| 7 |
Eg |
3106 |
2971 |
0.00 |
144.48 |
0.75 |
0.86 |
| 8 |
Eg |
1510 |
1444 |
0.00 |
24.89 |
0.75 |
0.86 |
| 8 |
Eg |
1510 |
1444 |
0.00 |
24.87 |
0.75 |
0.86 |
| 9 |
Eg |
1222 |
1169 |
0.00 |
0.84 |
0.75 |
0.86 |
| 9 |
Eg |
1222 |
1169 |
0.00 |
0.84 |
0.75 |
0.86 |
| 10 |
Eu |
3130 |
2993 |
70.47 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3130 |
2993 |
70.58 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1444 |
11.61 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1444 |
11.58 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
833 |
797 |
4.92 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
833 |
797 |
4.92 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16438.7 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 15723.6 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 wB97X-D/6-311G**
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 | | 1.5268 | 1.0931 | 1.0931 | 1.0931 | 2.1765 | 2.1765 | 2.1765 |
C2 | 1.5268 | | 2.1765 | 2.1765 | 2.1765 | 1.0931 | 1.0931 | 1.0931 | H3 | 1.0931 | 2.1765 | | 1.7643 | 1.7643 | 3.0876 | 2.5338 | 2.5338 | H4 | 1.0931 | 2.1765 | 1.7643 | | 1.7643 | 2.5338 | 2.5338 | 3.0876 | H5 | 1.0931 | 2.1765 | 1.7643 | 1.7643 | | 2.5338 | 3.0876 | 2.5338 | H6 | 2.1765 | 1.0931 | 3.0876 | 2.5338 | 2.5338 | | 1.7643 | 1.7643 | H7 | 2.1765 | 1.0931 | 2.5338 | 2.5338 | 3.0876 | 1.7643 | | 1.7643 | H8 | 2.1765 | 1.0931 | 2.5338 | 3.0876 | 2.5338 | 1.7643 | 1.7643 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.273 |
|
C1 |
C2 |
H7 |
111.273 |
| C1 |
C2 |
H8 |
111.273 |
|
C2 |
C1 |
H3 |
111.273 |
| C2 |
C1 |
H4 |
111.273 |
|
C2 |
C1 |
H5 |
111.273 |
| H3 |
C1 |
H4 |
107.610 |
|
H3 |
C1 |
H5 |
107.610 |
| H4 |
C1 |
H5 |
107.610 |
|
H6 |
C2 |
H7 |
107.610 |
| H6 |
C2 |
H8 |
107.610 |
|
H7 |
C2 |
H8 |
107.610 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.344 |
|
|
|
| 2 |
C |
-0.344 |
|
|
|
| 3 |
H |
0.115 |
|
|
|
| 4 |
H |
0.115 |
|
|
|
| 5 |
H |
0.115 |
|
|
|
| 6 |
H |
0.115 |
|
|
|
| 7 |
H |
0.115 |
|
|
|
| 8 |
H |
0.115 |
|
|
|
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 |
-14.832 |
0.000 |
0.000 |
| y |
0.000 |
-14.832 |
0.000 |
| z |
0.000 |
0.000 |
-15.469 |
|
| Traceless |
| | x | y | z |
| x |
0.318 |
0.000 |
0.000 |
| y |
0.000 |
0.318 |
0.000 |
| z |
0.000 |
0.000 |
-0.637 |
|
| Polar |
| 3z2-r2 | -1.273 |
| 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 |
3.614 |
0.000 |
| z |
0.000 |
0.000 |
3.970 |
<r2> (average value of r
2) Å
2
| <r2> |
30.690 |
| (<r2>)1/2 |
5.540 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -79.820481 |
| Energy at 298.15K | |
| HF Energy | -79.820481 |
| Nuclear repulsion energy | 42.059675 |
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 wB97X-D/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' |
3068 |
2934 |
0.00 |
|
|
|
| 2 |
A1' |
1453 |
1390 |
0.00 |
|
|
|
| 3 |
A1' |
1011 |
967 |
0.00 |
|
|
|
| 4 |
A1" |
294i |
281i |
0.00 |
|
|
|
| 5 |
A2" |
3059 |
2926 |
64.53 |
|
|
|
| 6 |
A2" |
1408 |
1347 |
2.68 |
|
|
|
| 7 |
E' |
3143 |
3006 |
59.63 |
|
|
|
| 7 |
E' |
3143 |
3006 |
59.82 |
|
|
|
| 8 |
E' |
1519 |
1453 |
13.80 |
|
|
|
| 8 |
E' |
1519 |
1453 |
13.75 |
|
|
|
| 9 |
E' |
910 |
870 |
4.41 |
|
|
|
| 9 |
E' |
910 |
870 |
4.44 |
|
|
|
| 10 |
E" |
3121 |
2985 |
0.00 |
|
|
|
| 10 |
E" |
3121 |
2985 |
0.00 |
|
|
|
| 11 |
E" |
1508 |
1442 |
0.00 |
|
|
|
| 11 |
E" |
1508 |
1442 |
0.00 |
|
|
|
| 12 |
E" |
1175 |
1124 |
0.00 |
|
|
|
| 12 |
E" |
1175 |
1124 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16228.4 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 15522.5 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 wB97X-D/6-311G**
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 |
1.174 |
| H4 |
-0.879 |
-0.507 |
1.174 |
| H5 |
0.879 |
-0.507 |
1.174 |
| H6 |
0.000 |
1.015 |
-1.174 |
| H7 |
0.879 |
-0.507 |
-1.174 |
| H8 |
-0.879 |
-0.507 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5406 | 1.0921 | 1.0921 | 1.0921 | 2.1932 | 2.1932 | 2.1932 |
C2 | 1.5406 | | 2.1932 | 2.1932 | 2.1932 | 1.0921 | 1.0921 | 1.0921 | H3 | 1.0921 | 2.1932 | | 1.7575 | 1.7575 | 2.3481 | 2.9330 | 2.9330 | H4 | 1.0921 | 2.1932 | 1.7575 | | 1.7575 | 2.9330 | 2.9330 | 2.3481 | H5 | 1.0921 | 2.1932 | 1.7575 | 1.7575 | | 2.9330 | 2.3481 | 2.9330 | H6 | 2.1932 | 1.0921 | 2.3481 | 2.9330 | 2.9330 | | 1.7575 | 1.7575 | H7 | 2.1932 | 1.0921 | 2.9330 | 2.9330 | 2.3481 | 1.7575 | | 1.7575 | H8 | 2.1932 | 1.0921 | 2.9330 | 2.3481 | 2.9330 | 1.7575 | 1.7575 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.698 |
|
C1 |
C2 |
H7 |
111.698 |
| C1 |
C2 |
H8 |
111.698 |
|
C2 |
C1 |
H3 |
111.698 |
| C2 |
C1 |
H4 |
111.698 |
|
C2 |
C1 |
H5 |
111.698 |
| H3 |
C1 |
H4 |
107.156 |
|
H3 |
C1 |
H5 |
107.156 |
| H4 |
C1 |
H5 |
107.156 |
|
H6 |
C2 |
H7 |
107.156 |
| H6 |
C2 |
H8 |
107.156 |
|
H7 |
C2 |
H8 |
107.156 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.358 |
|
|
|
| 2 |
C |
-0.358 |
|
|
|
| 3 |
H |
0.119 |
|
|
|
| 4 |
H |
0.119 |
|
|
|
| 5 |
H |
0.119 |
|
|
|
| 6 |
H |
0.119 |
|
|
|
| 7 |
H |
0.119 |
|
|
|
| 8 |
H |
0.119 |
|
|
|
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 |
-14.820 |
0.000 |
0.000 |
| y |
0.000 |
-14.820 |
0.000 |
| z |
0.000 |
0.000 |
-15.446 |
|
| Traceless |
| | x | y | z |
| x |
0.313 |
0.000 |
0.000 |
| y |
0.000 |
0.313 |
0.000 |
| z |
0.000 |
0.000 |
-0.626 |
|
| Polar |
| 3z2-r2 | -1.253 |
| 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 |
3.556 |
0.000 |
0.000 |
| y |
0.000 |
3.554 |
0.000 |
| z |
0.000 |
0.000 |
3.899 |
<r2> (average value of r
2) Å
2
| <r2> |
30.955 |
| (<r2>)1/2 |
5.564 |