Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.722392 |
| Energy at 298.15K | -79.728307 |
| HF Energy | -79.722392 |
| Nuclear repulsion energy | 42.112334 |
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 PBE1PBE/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 |
3058 |
2940 |
0.00 |
265.52 |
0.01 |
0.01 |
| 2 |
A1g |
1412 |
1358 |
0.00 |
3.72 |
0.75 |
0.85 |
| 3 |
A1g |
1039 |
999 |
0.00 |
9.65 |
0.28 |
0.44 |
| 4 |
A1u |
321 |
308 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3055 |
2937 |
56.06 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1380 |
1326 |
0.36 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3126 |
3006 |
0.00 |
153.37 |
0.75 |
0.86 |
| 7 |
Eg |
3126 |
3006 |
0.00 |
153.37 |
0.75 |
0.86 |
| 8 |
Eg |
1476 |
1419 |
0.00 |
29.16 |
0.75 |
0.86 |
| 8 |
Eg |
1476 |
1419 |
0.00 |
29.16 |
0.75 |
0.86 |
| 9 |
Eg |
1204 |
1157 |
0.00 |
0.70 |
0.75 |
0.86 |
| 9 |
Eg |
1204 |
1157 |
0.00 |
0.70 |
0.75 |
0.86 |
| 10 |
Eu |
3150 |
3029 |
51.22 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3150 |
3029 |
51.23 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1476 |
1419 |
9.51 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1476 |
1419 |
9.51 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
820 |
788 |
5.70 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
820 |
788 |
5.70 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16383.0 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15752.2 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 PBE1PBE/cc-pVDZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.760 |
| C2 |
0.000 |
0.000 |
-0.760 |
| H3 |
0.000 |
1.025 |
1.164 |
| H4 |
-0.887 |
-0.512 |
1.164 |
| H5 |
0.887 |
-0.512 |
1.164 |
| H6 |
0.000 |
-1.025 |
-1.164 |
| H7 |
-0.887 |
0.512 |
-1.164 |
| H8 |
0.887 |
0.512 |
-1.164 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5202 | 1.1015 | 1.1015 | 1.1015 | 2.1803 | 2.1803 | 2.1803 |
C2 | 1.5202 | | 2.1803 | 2.1803 | 2.1803 | 1.1015 | 1.1015 | 1.1015 | H3 | 1.1015 | 2.1803 | | 1.7747 | 1.7747 | 3.1021 | 2.5442 | 2.5442 | H4 | 1.1015 | 2.1803 | 1.7747 | | 1.7747 | 2.5442 | 2.5442 | 3.1021 | H5 | 1.1015 | 2.1803 | 1.7747 | 1.7747 | | 2.5442 | 3.1021 | 2.5442 | H6 | 2.1803 | 1.1015 | 3.1021 | 2.5442 | 2.5442 | | 1.7747 | 1.7747 | H7 | 2.1803 | 1.1015 | 2.5442 | 2.5442 | 3.1021 | 1.7747 | | 1.7747 | H8 | 2.1803 | 1.1015 | 2.5442 | 3.1021 | 2.5442 | 1.7747 | 1.7747 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.532 |
|
C1 |
C2 |
H7 |
111.532 |
| C1 |
C2 |
H8 |
111.532 |
|
C2 |
C1 |
H3 |
111.532 |
| C2 |
C1 |
H4 |
111.532 |
|
C2 |
C1 |
H5 |
111.532 |
| H3 |
C1 |
H4 |
107.334 |
|
H3 |
C1 |
H5 |
107.334 |
| H4 |
C1 |
H5 |
107.334 |
|
H6 |
C2 |
H7 |
107.334 |
| H6 |
C2 |
H8 |
107.334 |
|
H7 |
C2 |
H8 |
107.334 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.136 |
|
|
|
| 2 |
C |
-0.136 |
|
|
|
| 3 |
H |
0.045 |
|
|
|
| 4 |
H |
0.045 |
|
|
|
| 5 |
H |
0.045 |
|
|
|
| 6 |
H |
0.045 |
|
|
|
| 7 |
H |
0.045 |
|
|
|
| 8 |
H |
0.045 |
|
|
|
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 |
-14.736 |
0.000 |
0.000 |
| y |
0.000 |
-14.736 |
0.000 |
| z |
0.000 |
0.000 |
-15.309 |
|
| Traceless |
| | x | y | z |
| x |
0.287 |
0.000 |
0.000 |
| y |
0.000 |
0.287 |
0.000 |
| z |
0.000 |
0.000 |
-0.573 |
|
| Polar |
| 3z2-r2 | -1.147 |
| 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 |
3.509 |
0.000 |
0.000 |
| y |
0.000 |
3.509 |
0.000 |
| z |
0.000 |
0.000 |
3.899 |
<r2> (average value of r
2) Å
2
| <r2> |
30.691 |
| (<r2>)1/2 |
5.540 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.717648 |
| Energy at 298.15K | |
| HF Energy | -79.717648 |
| Nuclear repulsion energy | 41.957302 |
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 PBE1PBE/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' |
3072 |
2954 |
0.00 |
|
|
|
| 2 |
A1' |
1421 |
1366 |
0.00 |
|
|
|
| 3 |
A1' |
1038 |
998 |
0.00 |
|
|
|
| 4 |
A1" |
313i |
301i |
0.00 |
|
|
|
| 5 |
A2" |
3062 |
2944 |
58.03 |
|
|
|
| 6 |
A2" |
1375 |
1322 |
0.25 |
|
|
|
| 7 |
E' |
3155 |
3034 |
39.85 |
|
|
|
| 7 |
E' |
3155 |
3034 |
39.85 |
|
|
|
| 8 |
E' |
1478 |
1421 |
11.78 |
|
|
|
| 8 |
E' |
1478 |
1421 |
11.77 |
|
|
|
| 9 |
E' |
885 |
851 |
4.78 |
|
|
|
| 9 |
E' |
885 |
851 |
4.78 |
|
|
|
| 10 |
E" |
3135 |
3014 |
0.00 |
|
|
|
| 10 |
E" |
3135 |
3014 |
0.00 |
|
|
|
| 11 |
E" |
1472 |
1416 |
0.00 |
|
|
|
| 11 |
E" |
1472 |
1416 |
0.00 |
|
|
|
| 12 |
E" |
1153 |
1108 |
0.00 |
|
|
|
| 12 |
E" |
1153 |
1108 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16104.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 15484.9 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 PBE1PBE/cc-pVDZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.767 |
| C2 |
0.000 |
0.000 |
-0.767 |
| H3 |
0.000 |
1.020 |
1.179 |
| H4 |
-0.883 |
-0.510 |
1.179 |
| H5 |
0.883 |
-0.510 |
1.179 |
| H6 |
0.000 |
1.020 |
-1.179 |
| H7 |
0.883 |
-0.510 |
-1.179 |
| H8 |
-0.883 |
-0.510 |
-1.179 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5331 | 1.1004 | 1.1004 | 1.1004 | 2.1969 | 2.1969 | 2.1969 |
C2 | 1.5331 | | 2.1969 | 2.1969 | 2.1969 | 1.1004 | 1.1004 | 1.1004 | H3 | 1.1004 | 2.1969 | | 1.7670 | 1.7670 | 2.3582 | 2.9467 | 2.9467 | H4 | 1.1004 | 2.1969 | 1.7670 | | 1.7670 | 2.9467 | 2.9467 | 2.3582 | H5 | 1.1004 | 2.1969 | 1.7670 | 1.7670 | | 2.9467 | 2.3582 | 2.9467 | H6 | 2.1969 | 1.1004 | 2.3582 | 2.9467 | 2.9467 | | 1.7670 | 1.7670 | H7 | 2.1969 | 1.1004 | 2.9467 | 2.9467 | 2.3582 | 1.7670 | | 1.7670 | H8 | 2.1969 | 1.1004 | 2.9467 | 2.3582 | 2.9467 | 1.7670 | 1.7670 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
112.019 |
|
C1 |
C2 |
H7 |
112.019 |
| C1 |
C2 |
H8 |
112.019 |
|
C2 |
C1 |
H3 |
112.019 |
| C2 |
C1 |
H4 |
112.019 |
|
C2 |
C1 |
H5 |
112.019 |
| H3 |
C1 |
H4 |
106.808 |
|
H3 |
C1 |
H5 |
106.808 |
| H4 |
C1 |
H5 |
106.808 |
|
H6 |
C2 |
H7 |
106.808 |
| H6 |
C2 |
H8 |
106.808 |
|
H7 |
C2 |
H8 |
106.808 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.137 |
|
|
|
| 2 |
C |
-0.137 |
|
|
|
| 3 |
H |
0.046 |
|
|
|
| 4 |
H |
0.046 |
|
|
|
| 5 |
H |
0.046 |
|
|
|
| 6 |
H |
0.046 |
|
|
|
| 7 |
H |
0.046 |
|
|
|
| 8 |
H |
0.046 |
|
|
|
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 |
-14.726 |
0.000 |
0.000 |
| y |
0.000 |
-14.726 |
0.000 |
| z |
0.000 |
0.000 |
-15.291 |
|
| Traceless |
| | x | y | z |
| x |
0.283 |
0.000 |
0.000 |
| y |
0.000 |
0.283 |
0.000 |
| z |
0.000 |
0.000 |
-0.565 |
|
| Polar |
| 3z2-r2 | -1.130 |
| 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 |
3.436 |
0.000 |
0.000 |
| y |
0.000 |
3.436 |
0.000 |
| z |
0.000 |
0.000 |
3.842 |
<r2> (average value of r
2) Å
2
| <r2> |
30.952 |
| (<r2>)1/2 |
5.563 |