Jump to
S1C2
Energy calculated at HF/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.234945 |
| Energy at 298.15K | -79.240958 |
| HF Energy | -79.234945 |
| Nuclear repulsion energy | 42.252370 |
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 HF/cc-pVDZ
| 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 |
3179 |
2887 |
0.00 |
269.77 |
0.01 |
0.03 |
| 2 |
A1g |
1540 |
1399 |
0.00 |
1.47 |
0.50 |
0.67 |
| 3 |
A1g |
1062 |
965 |
0.00 |
14.98 |
0.28 |
0.44 |
| 4 |
A1u |
340 |
309 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3169 |
2877 |
76.02 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1502 |
1363 |
0.00 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3230 |
2933 |
0.00 |
168.58 |
0.75 |
0.86 |
| 7 |
Eg |
3230 |
2933 |
0.00 |
168.58 |
0.75 |
0.86 |
| 8 |
Eg |
1596 |
1449 |
0.00 |
27.39 |
0.75 |
0.86 |
| 8 |
Eg |
1596 |
1449 |
0.00 |
27.39 |
0.75 |
0.86 |
| 9 |
Eg |
1313 |
1192 |
0.00 |
0.96 |
0.75 |
0.86 |
| 9 |
Eg |
1313 |
1192 |
0.00 |
0.96 |
0.75 |
0.86 |
| 10 |
Eu |
3255 |
2956 |
93.89 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3255 |
2956 |
93.89 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1599 |
1452 |
7.01 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1599 |
1452 |
7.01 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
877 |
797 |
2.73 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
877 |
797 |
2.73 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17266.5 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 15678.0 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 HF/cc-pVDZ
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 |
1.159 |
| H4 |
-0.882 |
-0.509 |
1.159 |
| H5 |
0.882 |
-0.509 |
1.159 |
| H6 |
0.000 |
-1.019 |
-1.159 |
| H7 |
-0.882 |
0.509 |
-1.159 |
| H8 |
0.882 |
0.509 |
-1.159 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5251 | 1.0928 | 1.0928 | 1.0928 | 2.1745 | 2.1745 | 2.1745 |
C2 | 1.5251 | | 2.1745 | 2.1745 | 2.1745 | 1.0928 | 1.0928 | 1.0928 | H3 | 1.0928 | 2.1745 | | 1.7642 | 1.7642 | 3.0854 | 2.5313 | 2.5313 | H4 | 1.0928 | 2.1745 | 1.7642 | | 1.7642 | 2.5313 | 2.5313 | 3.0854 | H5 | 1.0928 | 2.1745 | 1.7642 | 1.7642 | | 2.5313 | 3.0854 | 2.5313 | H6 | 2.1745 | 1.0928 | 3.0854 | 2.5313 | 2.5313 | | 1.7642 | 1.7642 | H7 | 2.1745 | 1.0928 | 2.5313 | 2.5313 | 3.0854 | 1.7642 | | 1.7642 | H8 | 2.1745 | 1.0928 | 2.5313 | 3.0854 | 2.5313 | 1.7642 | 1.7642 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.250 |
|
C1 |
C2 |
H7 |
111.250 |
| C1 |
C2 |
H8 |
111.250 |
|
C2 |
C1 |
H3 |
111.250 |
| C2 |
C1 |
H4 |
111.250 |
|
C2 |
C1 |
H5 |
111.250 |
| H3 |
C1 |
H4 |
107.635 |
|
H3 |
C1 |
H5 |
107.635 |
| H4 |
C1 |
H5 |
107.635 |
|
H6 |
C2 |
H7 |
107.635 |
| H6 |
C2 |
H8 |
107.635 |
|
H7 |
C2 |
H8 |
107.635 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.090 |
|
|
|
| 2 |
C |
-0.090 |
|
|
|
| 3 |
H |
0.030 |
|
|
|
| 4 |
H |
0.030 |
|
|
|
| 5 |
H |
0.030 |
|
|
|
| 6 |
H |
0.030 |
|
|
|
| 7 |
H |
0.030 |
|
|
|
| 8 |
H |
0.030 |
|
|
|
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 |
-14.908 |
0.000 |
0.000 |
| y |
0.000 |
-14.908 |
0.000 |
| z |
0.000 |
0.000 |
-15.627 |
|
| Traceless |
| | x | y | z |
| x |
0.359 |
0.000 |
0.000 |
| y |
0.000 |
0.359 |
0.000 |
| z |
0.000 |
0.000 |
-0.719 |
|
| Polar |
| 3z2-r2 | -1.438 |
| 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 |
3.421 |
0.000 |
0.000 |
| y |
0.000 |
3.421 |
0.000 |
| z |
0.000 |
0.000 |
3.749 |
<r2> (average value of r
2) Å
2
| <r2> |
30.718 |
| (<r2>)1/2 |
5.542 |
Jump to
S1C1
Energy calculated at HF/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.229698 |
| Energy at 298.15K | |
| HF Energy | -79.229698 |
| Nuclear repulsion energy | 42.073012 |
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 HF/cc-pVDZ
| 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' |
3192 |
2898 |
0.00 |
|
|
|
| 2 |
A1' |
1549 |
1407 |
0.00 |
|
|
|
| 3 |
A1' |
1057 |
960 |
0.00 |
|
|
|
| 4 |
A1" |
330i |
299i |
0.00 |
|
|
|
| 5 |
A2" |
3175 |
2883 |
80.10 |
|
|
|
| 6 |
A2" |
1498 |
1360 |
0.03 |
|
|
|
| 7 |
E' |
3262 |
2961 |
78.38 |
|
|
|
| 7 |
E' |
3262 |
2961 |
78.38 |
|
|
|
| 8 |
E' |
1603 |
1456 |
9.12 |
|
|
|
| 8 |
E' |
1603 |
1456 |
9.12 |
|
|
|
| 9 |
E' |
949 |
862 |
2.34 |
|
|
|
| 9 |
E' |
949 |
862 |
2.34 |
|
|
|
| 10 |
E" |
3237 |
2939 |
0.00 |
|
|
|
| 10 |
E" |
3237 |
2939 |
0.00 |
|
|
|
| 11 |
E" |
1593 |
1446 |
0.00 |
|
|
|
| 11 |
E" |
1593 |
1446 |
0.00 |
|
|
|
| 12 |
E" |
1264 |
1147 |
0.00 |
|
|
|
| 12 |
E" |
1264 |
1147 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16977.8 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 15415.9 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 HF/cc-pVDZ
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 |
1.014 |
1.174 |
| H4 |
-0.878 |
-0.507 |
1.174 |
| H5 |
0.878 |
-0.507 |
1.174 |
| H6 |
0.000 |
1.014 |
-1.174 |
| H7 |
0.878 |
-0.507 |
-1.174 |
| H8 |
-0.878 |
-0.507 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5400 | 1.0918 | 1.0918 | 1.0918 | 2.1926 | 2.1926 | 2.1926 |
C2 | 1.5400 | | 2.1926 | 2.1926 | 2.1926 | 1.0918 | 1.0918 | 1.0918 | H3 | 1.0918 | 2.1926 | | 1.7569 | 1.7569 | 2.3478 | 2.9324 | 2.9324 | H4 | 1.0918 | 2.1926 | 1.7569 | | 1.7569 | 2.9324 | 2.9324 | 2.3478 | H5 | 1.0918 | 2.1926 | 1.7569 | 1.7569 | | 2.9324 | 2.3478 | 2.9324 | H6 | 2.1926 | 1.0918 | 2.3478 | 2.9324 | 2.9324 | | 1.7569 | 1.7569 | H7 | 2.1926 | 1.0918 | 2.9324 | 2.9324 | 2.3478 | 1.7569 | | 1.7569 | H8 | 2.1926 | 1.0918 | 2.9324 | 2.3478 | 2.9324 | 1.7569 | 1.7569 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.712 |
|
C1 |
C2 |
H7 |
111.712 |
| C1 |
C2 |
H8 |
111.712 |
|
C2 |
C1 |
H3 |
111.712 |
| C2 |
C1 |
H4 |
111.712 |
|
C2 |
C1 |
H5 |
111.712 |
| H3 |
C1 |
H4 |
107.141 |
|
H3 |
C1 |
H5 |
107.141 |
| H4 |
C1 |
H5 |
107.141 |
|
H6 |
C2 |
H7 |
107.141 |
| H6 |
C2 |
H8 |
107.141 |
|
H7 |
C2 |
H8 |
107.141 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.096 |
|
|
|
| 2 |
C |
-0.096 |
|
|
|
| 3 |
H |
0.032 |
|
|
|
| 4 |
H |
0.032 |
|
|
|
| 5 |
H |
0.032 |
|
|
|
| 6 |
H |
0.032 |
|
|
|
| 7 |
H |
0.032 |
|
|
|
| 8 |
H |
0.032 |
|
|
|
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 |
-14.892 |
0.000 |
0.000 |
| y |
0.000 |
-14.892 |
0.000 |
| z |
0.000 |
0.000 |
-15.598 |
|
| Traceless |
| | x | y | z |
| x |
0.353 |
0.000 |
0.000 |
| y |
0.000 |
0.353 |
0.000 |
| z |
0.000 |
0.000 |
-0.706 |
|
| Polar |
| 3z2-r2 | -1.412 |
| 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 |
3.356 |
0.000 |
0.000 |
| y |
0.000 |
3.356 |
0.000 |
| z |
0.000 |
0.000 |
3.721 |
<r2> (average value of r
2) Å
2
| <r2> |
31.005 |
| (<r2>)1/2 |
5.568 |