Jump to
S1C2
Energy calculated at B3LYP/TZVP
| | hartrees |
| Energy at 0K | -79.862337 |
| Energy at 298.15K | -79.868249 |
| HF Energy | -79.862337 |
| Nuclear repulsion energy | 42.217732 |
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 B3LYP/TZVP
| 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 |
3030 |
2925 |
0.00 |
289.43 |
0.01 |
0.02 |
| 2 |
A1g |
1429 |
1380 |
0.00 |
2.16 |
0.73 |
0.84 |
| 3 |
A1g |
996 |
961 |
0.00 |
11.69 |
0.25 |
0.40 |
| 4 |
A1u |
309 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3031 |
2926 |
61.56 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1415 |
1366 |
1.73 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3076 |
2970 |
0.00 |
145.08 |
0.75 |
0.86 |
| 7 |
Eg |
3076 |
2970 |
0.00 |
145.08 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1455 |
0.00 |
26.82 |
0.75 |
0.86 |
| 8 |
Eg |
1507 |
1455 |
0.00 |
26.82 |
0.75 |
0.86 |
| 9 |
Eg |
1224 |
1181 |
0.00 |
0.74 |
0.75 |
0.86 |
| 9 |
Eg |
1224 |
1181 |
0.00 |
0.74 |
0.75 |
0.86 |
| 10 |
Eu |
3101 |
2994 |
70.68 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3101 |
2994 |
70.68 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1457 |
10.93 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1457 |
10.93 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
830 |
802 |
3.76 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
830 |
802 |
3.76 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16351.8 cm
-1
Scaled (by 0.9654) Zero Point Vibrational Energy (zpe) 15786.0 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 B3LYP/TZVP
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.764 |
| C2 |
0.000 |
0.000 |
-0.764 |
| H3 |
0.000 |
1.017 |
1.162 |
| H4 |
-0.881 |
-0.509 |
1.162 |
| H5 |
0.881 |
-0.509 |
1.162 |
| H6 |
0.000 |
-1.017 |
-1.162 |
| H7 |
-0.881 |
0.509 |
-1.162 |
| H8 |
0.881 |
0.509 |
-1.162 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5283 | 1.0923 | 1.0923 | 1.0923 | 2.1783 | 2.1783 | 2.1783 |
C2 | 1.5283 | | 2.1783 | 2.1783 | 2.1783 | 1.0923 | 1.0923 | 1.0923 | H3 | 1.0923 | 2.1783 | | 1.7621 | 1.7621 | 3.0887 | 2.5368 | 2.5368 | H4 | 1.0923 | 2.1783 | 1.7621 | | 1.7621 | 2.5368 | 2.5368 | 3.0887 | H5 | 1.0923 | 2.1783 | 1.7621 | 1.7621 | | 2.5368 | 3.0887 | 2.5368 | H6 | 2.1783 | 1.0923 | 3.0887 | 2.5368 | 2.5368 | | 1.7621 | 1.7621 | H7 | 2.1783 | 1.0923 | 2.5368 | 2.5368 | 3.0887 | 1.7621 | | 1.7621 | H8 | 2.1783 | 1.0923 | 2.5368 | 3.0887 | 2.5368 | 1.7621 | 1.7621 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.354 |
|
C1 |
C2 |
H7 |
111.354 |
| C1 |
C2 |
H8 |
111.354 |
|
C2 |
C1 |
H3 |
111.354 |
| C2 |
C1 |
H4 |
111.354 |
|
C2 |
C1 |
H5 |
111.354 |
| H3 |
C1 |
H4 |
107.524 |
|
H3 |
C1 |
H5 |
107.524 |
| H4 |
C1 |
H5 |
107.524 |
|
H6 |
C2 |
H7 |
107.524 |
| H6 |
C2 |
H8 |
107.524 |
|
H7 |
C2 |
H8 |
107.524 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.331 |
|
|
|
| 2 |
C |
-0.331 |
|
|
|
| 3 |
H |
0.110 |
|
|
|
| 4 |
H |
0.110 |
|
|
|
| 5 |
H |
0.110 |
|
|
|
| 6 |
H |
0.110 |
|
|
|
| 7 |
H |
0.110 |
|
|
|
| 8 |
H |
0.110 |
|
|
|
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 |
-15.060 |
0.000 |
0.000 |
| y |
0.000 |
-15.060 |
0.000 |
| z |
0.000 |
0.000 |
-15.754 |
|
| Traceless |
| | x | y | z |
| x |
0.347 |
0.000 |
0.000 |
| y |
0.000 |
0.347 |
0.000 |
| z |
0.000 |
0.000 |
-0.694 |
|
| Polar |
| 3z2-r2 | -1.387 |
| 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 |
3.813 |
0.000 |
0.000 |
| y |
0.000 |
3.813 |
0.000 |
| z |
0.000 |
0.000 |
4.168 |
<r2> (average value of r
2) Å
2
| <r2> |
30.869 |
| (<r2>)1/2 |
5.556 |
Jump to
S1C1
Energy calculated at B3LYP/TZVP
| | hartrees |
| Energy at 0K | -79.858021 |
| Energy at 298.15K | |
| HF Energy | -79.858021 |
| Nuclear repulsion energy | 42.053336 |
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 B3LYP/TZVP
| 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' |
3046 |
2940 |
0.00 |
|
|
|
| 2 |
A1' |
1447 |
1397 |
0.00 |
|
|
|
| 3 |
A1' |
991 |
957 |
0.00 |
|
|
|
| 4 |
A1" |
300i |
289i |
0.00 |
|
|
|
| 5 |
A2" |
3039 |
2934 |
66.21 |
|
|
|
| 6 |
A2" |
1413 |
1364 |
2.03 |
|
|
|
| 7 |
E' |
3109 |
3001 |
58.98 |
|
|
|
| 7 |
E' |
3109 |
3001 |
58.98 |
|
|
|
| 8 |
E' |
1515 |
1462 |
13.43 |
|
|
|
| 8 |
E' |
1515 |
1462 |
13.43 |
|
|
|
| 9 |
E' |
901 |
870 |
3.46 |
|
|
|
| 9 |
E' |
901 |
870 |
3.46 |
|
|
|
| 10 |
E" |
3086 |
2979 |
0.00 |
|
|
|
| 10 |
E" |
3086 |
2979 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1453 |
0.00 |
|
|
|
| 11 |
E" |
1505 |
1453 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1134 |
0.00 |
|
|
|
| 12 |
E" |
1174 |
1134 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16107.6 cm
-1
Scaled (by 0.9654) Zero Point Vibrational Energy (zpe) 15550.3 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 B3LYP/TZVP
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.771 |
| C2 |
0.000 |
0.000 |
-0.771 |
| H3 |
0.000 |
1.013 |
1.177 |
| H4 |
-0.877 |
-0.507 |
1.177 |
| H5 |
0.877 |
-0.507 |
1.177 |
| H6 |
0.000 |
1.013 |
-1.177 |
| H7 |
0.877 |
-0.507 |
-1.177 |
| H8 |
-0.877 |
-0.507 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5422 | 1.0912 | 1.0912 | 1.0912 | 2.1954 | 2.1954 | 2.1954 |
C2 | 1.5422 | | 2.1954 | 2.1954 | 2.1954 | 1.0912 | 1.0912 | 1.0912 | H3 | 1.0912 | 2.1954 | | 1.7548 | 1.7548 | 2.3530 | 2.9353 | 2.9353 | H4 | 1.0912 | 2.1954 | 1.7548 | | 1.7548 | 2.9353 | 2.9353 | 2.3530 | H5 | 1.0912 | 2.1954 | 1.7548 | 1.7548 | | 2.9353 | 2.3530 | 2.9353 | H6 | 2.1954 | 1.0912 | 2.3530 | 2.9353 | 2.9353 | | 1.7548 | 1.7548 | H7 | 2.1954 | 1.0912 | 2.9353 | 2.9353 | 2.3530 | 1.7548 | | 1.7548 | H8 | 2.1954 | 1.0912 | 2.9353 | 2.3530 | 2.9353 | 1.7548 | 1.7548 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.809 |
|
C1 |
C2 |
H7 |
111.809 |
| C1 |
C2 |
H8 |
111.809 |
|
C2 |
C1 |
H3 |
111.809 |
| C2 |
C1 |
H4 |
111.809 |
|
C2 |
C1 |
H5 |
111.809 |
| H3 |
C1 |
H4 |
107.036 |
|
H3 |
C1 |
H5 |
107.036 |
| H4 |
C1 |
H5 |
107.036 |
|
H6 |
C2 |
H7 |
107.036 |
| H6 |
C2 |
H8 |
107.036 |
|
H7 |
C2 |
H8 |
107.036 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.351 |
|
|
|
| 2 |
C |
-0.351 |
|
|
|
| 3 |
H |
0.117 |
|
|
|
| 4 |
H |
0.117 |
|
|
|
| 5 |
H |
0.117 |
|
|
|
| 6 |
H |
0.117 |
|
|
|
| 7 |
H |
0.117 |
|
|
|
| 8 |
H |
0.117 |
|
|
|
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 |
-15.044 |
0.000 |
0.000 |
| y |
0.000 |
-15.044 |
0.000 |
| z |
0.000 |
0.000 |
-15.741 |
|
| Traceless |
| | x | y | z |
| x |
0.349 |
0.000 |
0.000 |
| y |
0.000 |
0.349 |
0.000 |
| z |
0.000 |
0.000 |
-0.697 |
|
| Polar |
| 3z2-r2 | -1.395 |
| 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 |
3.775 |
0.000 |
0.000 |
| y |
0.000 |
3.775 |
0.000 |
| z |
0.000 |
0.000 |
3.981 |
<r2> (average value of r
2) Å
2
| <r2> |
31.141 |
| (<r2>)1/2 |
5.580 |