Jump to
S1C2
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.771045 |
| Energy at 298.15K | -79.776906 |
| HF Energy | -79.771045 |
| Nuclear repulsion energy | 41.863240 |
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 BLYP/6-31G(2df,p)
| 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 |
2960 |
2944 |
0.00 |
211.10 |
0.01 |
0.01 |
| 2 |
A1g |
1382 |
1374 |
0.00 |
7.49 |
0.68 |
0.81 |
| 3 |
A1g |
969 |
963 |
0.00 |
8.54 |
0.27 |
0.43 |
| 4 |
A1u |
303 |
301 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
2963 |
2947 |
58.74 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1374 |
1367 |
0.18 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3008 |
2991 |
0.00 |
127.85 |
0.75 |
0.86 |
| 7 |
Eg |
3008 |
2991 |
0.00 |
127.85 |
0.75 |
0.86 |
| 8 |
Eg |
1466 |
1458 |
0.00 |
33.18 |
0.75 |
0.86 |
| 8 |
Eg |
1466 |
1458 |
0.00 |
33.18 |
0.75 |
0.86 |
| 9 |
Eg |
1189 |
1183 |
0.00 |
2.25 |
0.75 |
0.86 |
| 9 |
Eg |
1189 |
1183 |
0.00 |
2.25 |
0.75 |
0.86 |
| 10 |
Eu |
3033 |
3017 |
68.59 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3033 |
3017 |
68.59 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1472 |
1464 |
4.62 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1472 |
1464 |
4.61 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
804 |
799 |
3.59 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
804 |
799 |
3.59 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 15947.6 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 15859.9 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 BLYP/6-31G(2df,p)
Point Group is D3d
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 |
1.026 |
1.172 |
| H4 |
-0.888 |
-0.513 |
1.172 |
| H5 |
0.888 |
-0.513 |
1.172 |
| H6 |
0.000 |
-1.026 |
-1.172 |
| H7 |
-0.888 |
0.513 |
-1.172 |
| H8 |
0.888 |
0.513 |
-1.172 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5408 | 1.1018 | 1.1018 | 1.1018 | 2.1970 | 2.1970 | 2.1970 |
C2 | 1.5408 | | 2.1970 | 2.1970 | 2.1970 | 1.1018 | 1.1018 | 1.1018 | H3 | 1.1018 | 2.1970 | | 1.7768 | 1.7768 | 3.1156 | 2.5593 | 2.5593 | H4 | 1.1018 | 2.1970 | 1.7768 | | 1.7768 | 2.5593 | 2.5593 | 3.1156 | H5 | 1.1018 | 2.1970 | 1.7768 | 1.7768 | | 2.5593 | 3.1156 | 2.5593 | H6 | 2.1970 | 1.1018 | 3.1156 | 2.5593 | 2.5593 | | 1.7768 | 1.7768 | H7 | 2.1970 | 1.1018 | 2.5593 | 2.5593 | 3.1156 | 1.7768 | | 1.7768 | H8 | 2.1970 | 1.1018 | 2.5593 | 3.1156 | 2.5593 | 1.7768 | 1.7768 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.398 |
|
C1 |
C2 |
H7 |
111.398 |
| C1 |
C2 |
H8 |
111.398 |
|
C2 |
C1 |
H3 |
111.398 |
| C2 |
C1 |
H4 |
111.398 |
|
C2 |
C1 |
H5 |
111.398 |
| H3 |
C1 |
H4 |
107.477 |
|
H3 |
C1 |
H5 |
107.477 |
| H4 |
C1 |
H5 |
107.477 |
|
H6 |
C2 |
H7 |
107.477 |
| H6 |
C2 |
H8 |
107.477 |
|
H7 |
C2 |
H8 |
107.477 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.302 |
|
|
|
| 2 |
C |
-0.302 |
|
|
|
| 3 |
H |
0.101 |
|
|
|
| 4 |
H |
0.101 |
|
|
|
| 5 |
H |
0.101 |
|
|
|
| 6 |
H |
0.101 |
|
|
|
| 7 |
H |
0.101 |
|
|
|
| 8 |
H |
0.101 |
|
|
|
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 |
-14.743 |
0.000 |
0.000 |
| y |
0.000 |
-14.743 |
0.000 |
| z |
0.000 |
0.000 |
-15.267 |
|
| Traceless |
| | x | y | z |
| x |
0.262 |
0.000 |
0.000 |
| y |
0.000 |
0.262 |
0.000 |
| z |
0.000 |
0.000 |
-0.525 |
|
| Polar |
| 3z2-r2 | -1.049 |
| 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 |
3.506 |
0.000 |
0.000 |
| y |
0.000 |
3.506 |
0.000 |
| z |
0.000 |
0.000 |
3.858 |
<r2> (average value of r
2) Å
2
| <r2> |
31.000 |
| (<r2>)1/2 |
5.568 |
Jump to
S1C1
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.766804 |
| Energy at 298.15K | |
| HF Energy | -79.766804 |
| Nuclear repulsion energy | 41.694286 |
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 BLYP/6-31G(2df,p)
| 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' |
2978 |
2961 |
0.00 |
|
|
|
| 2 |
A1' |
1400 |
1392 |
0.00 |
|
|
|
| 3 |
A1' |
963 |
958 |
0.00 |
|
|
|
| 4 |
A1" |
296i |
294i |
0.00 |
|
|
|
| 5 |
A2" |
2972 |
2956 |
60.15 |
|
|
|
| 6 |
A2" |
1371 |
1363 |
0.39 |
|
|
|
| 7 |
E' |
3042 |
3026 |
57.36 |
|
|
|
| 7 |
E' |
3042 |
3026 |
57.36 |
|
|
|
| 8 |
E' |
1474 |
1466 |
5.69 |
|
|
|
| 8 |
E' |
1474 |
1466 |
5.69 |
|
|
|
| 9 |
E' |
876 |
871 |
2.88 |
|
|
|
| 9 |
E' |
876 |
871 |
2.88 |
|
|
|
| 10 |
E" |
3020 |
3003 |
0.00 |
|
|
|
| 10 |
E" |
3020 |
3003 |
0.00 |
|
|
|
| 11 |
E" |
1468 |
1460 |
0.00 |
|
|
|
| 11 |
E" |
1468 |
1460 |
0.00 |
|
|
|
| 12 |
E" |
1142 |
1136 |
0.00 |
|
|
|
| 12 |
E" |
1142 |
1136 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15715.1 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 15628.6 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 BLYP/6-31G(2df,p)
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.778 |
| C2 |
0.000 |
0.000 |
-0.778 |
| H3 |
0.000 |
1.022 |
1.187 |
| H4 |
-0.885 |
-0.511 |
1.187 |
| H5 |
0.885 |
-0.511 |
1.187 |
| H6 |
0.000 |
1.022 |
-1.187 |
| H7 |
0.885 |
-0.511 |
-1.187 |
| H8 |
-0.885 |
-0.511 |
-1.187 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5557 | 1.1005 | 1.1005 | 1.1005 | 2.2145 | 2.2145 | 2.2145 |
C2 | 1.5557 | | 2.2145 | 2.2145 | 2.2145 | 1.1005 | 1.1005 | 1.1005 | H3 | 1.1005 | 2.2145 | | 1.7695 | 1.7695 | 2.3739 | 2.9608 | 2.9608 | H4 | 1.1005 | 2.2145 | 1.7695 | | 1.7695 | 2.9608 | 2.9608 | 2.3739 | H5 | 1.1005 | 2.2145 | 1.7695 | 1.7695 | | 2.9608 | 2.3739 | 2.9608 | H6 | 2.2145 | 1.1005 | 2.3739 | 2.9608 | 2.9608 | | 1.7695 | 1.7695 | H7 | 2.2145 | 1.1005 | 2.9608 | 2.9608 | 2.3739 | 1.7695 | | 1.7695 | H8 | 2.2145 | 1.1005 | 2.9608 | 2.3739 | 2.9608 | 1.7695 | 1.7695 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.822 |
|
C1 |
C2 |
H7 |
111.822 |
| C1 |
C2 |
H8 |
111.822 |
|
C2 |
C1 |
H3 |
111.822 |
| C2 |
C1 |
H4 |
111.822 |
|
C2 |
C1 |
H5 |
111.822 |
| H3 |
C1 |
H4 |
107.021 |
|
H3 |
C1 |
H5 |
107.021 |
| H4 |
C1 |
H5 |
107.021 |
|
H6 |
C2 |
H7 |
107.021 |
| H6 |
C2 |
H8 |
107.021 |
|
H7 |
C2 |
H8 |
107.021 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.310 |
|
|
|
| 2 |
C |
-0.310 |
|
|
|
| 3 |
H |
0.103 |
|
|
|
| 4 |
H |
0.103 |
|
|
|
| 5 |
H |
0.103 |
|
|
|
| 6 |
H |
0.103 |
|
|
|
| 7 |
H |
0.103 |
|
|
|
| 8 |
H |
0.103 |
|
|
|
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 |
-14.720 |
0.000 |
0.000 |
| y |
0.000 |
-14.720 |
0.000 |
| z |
0.000 |
0.000 |
-15.242 |
|
| Traceless |
| | x | y | z |
| x |
0.261 |
0.000 |
0.000 |
| y |
0.000 |
0.261 |
0.000 |
| z |
0.000 |
0.000 |
-0.523 |
|
| Polar |
| 3z2-r2 | -1.045 |
| 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 |
3.449 |
0.000 |
0.000 |
| y |
0.000 |
3.449 |
0.000 |
| z |
0.000 |
0.000 |
3.824 |
<r2> (average value of r
2) Å
2
| <r2> |
31.279 |
| (<r2>)1/2 |
5.593 |