Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.781115 |
| Energy at 298.15K | |
| HF Energy | -79.651920 |
| Nuclear repulsion energy | 42.364414 |
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 B2PLYP=FULLultrafine/cc-pVTZ
| 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 |
3059 |
2922 |
0.00 |
286.19 |
0.01 |
0.01 |
| 2 |
A1g |
1437 |
1373 |
0.00 |
0.70 |
0.74 |
0.85 |
| 3 |
A1g |
1012 |
967 |
0.00 |
11.70 |
0.22 |
0.36 |
| 4 |
A1u |
317 |
303 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3060 |
2923 |
56.66 |
0.00 |
0.01 |
0.01 |
| 6 |
A2u |
1422 |
1359 |
1.07 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3108 |
2969 |
0.00 |
131.00 |
0.75 |
0.86 |
| 7 |
Eg |
3108 |
2969 |
0.00 |
130.99 |
0.75 |
0.86 |
| 8 |
Eg |
1522 |
1454 |
0.00 |
17.27 |
0.75 |
0.86 |
| 8 |
Eg |
1522 |
1454 |
0.00 |
17.27 |
0.75 |
0.86 |
| 9 |
Eg |
1235 |
1180 |
0.00 |
0.29 |
0.75 |
0.86 |
| 9 |
Eg |
1235 |
1180 |
0.00 |
0.29 |
0.75 |
0.86 |
| 10 |
Eu |
3132 |
2992 |
62.40 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3132 |
2992 |
62.40 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1524 |
1456 |
8.42 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1524 |
1456 |
8.42 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
795 |
3.50 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
832 |
795 |
3.50 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16505.0 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 15768.9 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 B2PLYP=FULLultrafine/cc-pVTZ
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 |
1.014 |
1.157 |
| H4 |
-0.878 |
-0.507 |
1.157 |
| H5 |
0.878 |
-0.507 |
1.157 |
| H6 |
0.000 |
-1.014 |
-1.157 |
| H7 |
-0.878 |
0.507 |
-1.157 |
| H8 |
0.878 |
0.507 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5240 | 1.0882 | 1.0882 | 1.0882 | 2.1703 | 2.1703 | 2.1703 |
C2 | 1.5240 | | 2.1703 | 2.1703 | 2.1703 | 1.0882 | 1.0882 | 1.0882 | H3 | 1.0882 | 2.1703 | | 1.7565 | 1.7565 | 3.0767 | 2.5261 | 2.5261 | H4 | 1.0882 | 2.1703 | 1.7565 | | 1.7565 | 2.5261 | 2.5261 | 3.0767 | H5 | 1.0882 | 2.1703 | 1.7565 | 1.7565 | | 2.5261 | 3.0767 | 2.5261 | H6 | 2.1703 | 1.0882 | 3.0767 | 2.5261 | 2.5261 | | 1.7565 | 1.7565 | H7 | 2.1703 | 1.0882 | 2.5261 | 2.5261 | 3.0767 | 1.7565 | | 1.7565 | H8 | 2.1703 | 1.0882 | 2.5261 | 3.0767 | 2.5261 | 1.7565 | 1.7565 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.272 |
|
C1 |
C2 |
H7 |
111.272 |
| C1 |
C2 |
H8 |
111.272 |
|
C2 |
C1 |
H3 |
111.272 |
| C2 |
C1 |
H4 |
111.272 |
|
C2 |
C1 |
H5 |
111.272 |
| H3 |
C1 |
H4 |
107.612 |
|
H3 |
C1 |
H5 |
107.612 |
| H4 |
C1 |
H5 |
107.612 |
|
H6 |
C2 |
H7 |
107.612 |
| H6 |
C2 |
H8 |
107.612 |
|
H7 |
C2 |
H8 |
107.612 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.312 |
|
|
|
| 2 |
C |
-0.312 |
|
|
|
| 3 |
H |
0.104 |
|
|
|
| 4 |
H |
0.104 |
|
|
|
| 5 |
H |
0.104 |
|
|
|
| 6 |
H |
0.104 |
|
|
|
| 7 |
H |
0.104 |
|
|
|
| 8 |
H |
0.104 |
|
|
|
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 |
-14.995 |
0.000 |
0.000 |
| y |
0.000 |
-14.995 |
0.000 |
| z |
0.000 |
0.000 |
-15.712 |
|
| Traceless |
| | x | y | z |
| x |
0.359 |
0.000 |
0.000 |
| y |
0.000 |
0.359 |
0.000 |
| z |
0.000 |
0.000 |
-0.718 |
|
| Polar |
| 3z2-r2 | -1.435 |
| 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 |
3.815 |
0.000 |
0.000 |
| y |
0.000 |
3.815 |
0.000 |
| z |
0.000 |
0.000 |
4.286 |
<r2> (average value of r
2) Å
2
| <r2> |
30.682 |
| (<r2>)1/2 |
5.539 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/cc-pVTZ
| | hartrees |
| Energy at 0K | -79.776658 |
| Energy at 298.15K | |
| HF Energy | -79.647450 |
| Nuclear repulsion energy | 42.199082 |
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 B2PLYP=FULLultrafine/cc-pVTZ
| 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' |
3074 |
2937 |
0.00 |
266.21 |
0.01 |
0.01 |
| 2 |
A1' |
1451 |
1386 |
0.00 |
0.61 |
0.74 |
0.85 |
| 3 |
A1' |
1008 |
963 |
0.00 |
14.07 |
0.19 |
0.32 |
| 4 |
A1" |
302i |
289i |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2" |
3067 |
2930 |
58.20 |
0.00 |
0.75 |
0.86 |
| 6 |
A2" |
1419 |
1356 |
0.73 |
0.00 |
0.75 |
0.86 |
| 7 |
E' |
3139 |
2999 |
52.69 |
52.06 |
0.75 |
0.86 |
| 7 |
E' |
3139 |
2999 |
52.69 |
52.06 |
0.75 |
0.86 |
| 8 |
E' |
1529 |
1461 |
9.88 |
3.19 |
0.75 |
0.86 |
| 8 |
E' |
1529 |
1461 |
9.88 |
3.19 |
0.75 |
0.86 |
| 9 |
E' |
904 |
864 |
2.58 |
0.00 |
0.75 |
0.86 |
| 9 |
E' |
904 |
864 |
2.58 |
0.00 |
0.75 |
0.86 |
| 10 |
E" |
3116 |
2977 |
0.00 |
63.30 |
0.75 |
0.86 |
| 10 |
E" |
3116 |
2977 |
0.00 |
63.30 |
0.75 |
0.86 |
| 11 |
E" |
1520 |
1452 |
0.00 |
11.83 |
0.75 |
0.86 |
| 11 |
E" |
1520 |
1452 |
0.00 |
11.83 |
0.75 |
0.86 |
| 12 |
E" |
1185 |
1132 |
0.00 |
0.99 |
0.75 |
0.86 |
| 12 |
E" |
1185 |
1132 |
0.00 |
0.99 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 16251.3 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 15526.5 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 B2PLYP=FULLultrafine/cc-pVTZ
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 |
1.010 |
1.171 |
| H4 |
-0.875 |
-0.505 |
1.171 |
| H5 |
0.875 |
-0.505 |
1.171 |
| H6 |
0.000 |
1.010 |
-1.171 |
| H7 |
0.875 |
-0.505 |
-1.171 |
| H8 |
-0.875 |
-0.505 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5381 | 1.0871 | 1.0871 | 1.0871 | 2.1872 | 2.1872 | 2.1872 |
C2 | 1.5381 | | 2.1872 | 2.1872 | 2.1872 | 1.0871 | 1.0871 | 1.0871 | H3 | 1.0871 | 2.1872 | | 1.7495 | 1.7495 | 2.3418 | 2.9232 | 2.9232 | H4 | 1.0871 | 2.1872 | 1.7495 | | 1.7495 | 2.9232 | 2.9232 | 2.3418 | H5 | 1.0871 | 2.1872 | 1.7495 | 1.7495 | | 2.9232 | 2.3418 | 2.9232 | H6 | 2.1872 | 1.0871 | 2.3418 | 2.9232 | 2.9232 | | 1.7495 | 1.7495 | H7 | 2.1872 | 1.0871 | 2.9232 | 2.9232 | 2.3418 | 1.7495 | | 1.7495 | H8 | 2.1872 | 1.0871 | 2.9232 | 2.3418 | 2.9232 | 1.7495 | 1.7495 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.696 |
|
C1 |
C2 |
H7 |
111.696 |
| C1 |
C2 |
H8 |
111.696 |
|
C2 |
C1 |
H3 |
111.696 |
| C2 |
C1 |
H4 |
111.696 |
|
C2 |
C1 |
H5 |
111.696 |
| H3 |
C1 |
H4 |
107.158 |
|
H3 |
C1 |
H5 |
107.158 |
| H4 |
C1 |
H5 |
107.158 |
|
H6 |
C2 |
H7 |
107.158 |
| H6 |
C2 |
H8 |
107.158 |
|
H7 |
C2 |
H8 |
107.158 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.320 |
|
|
|
| 2 |
C |
-0.320 |
|
|
|
| 3 |
H |
0.107 |
|
|
|
| 4 |
H |
0.107 |
|
|
|
| 5 |
H |
0.107 |
|
|
|
| 6 |
H |
0.107 |
|
|
|
| 7 |
H |
0.107 |
|
|
|
| 8 |
H |
0.107 |
|
|
|
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 |
-14.980 |
0.000 |
0.000 |
| y |
0.000 |
-14.980 |
0.000 |
| z |
0.000 |
0.000 |
-15.692 |
|
| Traceless |
| | x | y | z |
| x |
0.356 |
0.000 |
0.000 |
| y |
0.000 |
0.356 |
0.000 |
| z |
0.000 |
0.000 |
-0.712 |
|
| Polar |
| 3z2-r2 | -1.424 |
| 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 |
3.776 |
0.000 |
0.000 |
| y |
0.000 |
3.776 |
0.000 |
| z |
0.000 |
0.000 |
4.250 |
<r2> (average value of r
2) Å
2
| <r2> |
30.949 |
| (<r2>)1/2 |
5.563 |