Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -79.777013 |
| Energy at 298.15K | -79.782921 |
| HF Energy | -79.777013 |
| Nuclear repulsion energy | 42.298849 |
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 B1B95/6-31+G**
| 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 |
3068 |
2935 |
0.00 |
262.93 |
0.01 |
0.02 |
| 2 |
A1g |
1433 |
1371 |
0.00 |
2.29 |
0.58 |
0.74 |
| 3 |
A1g |
1027 |
982 |
0.00 |
12.80 |
0.29 |
0.44 |
| 4 |
A1u |
313 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3067 |
2934 |
64.74 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1404 |
1343 |
2.20 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3132 |
2996 |
0.00 |
143.04 |
0.75 |
0.86 |
| 7 |
Eg |
3132 |
2996 |
0.00 |
143.04 |
0.75 |
0.86 |
| 8 |
Eg |
1509 |
1444 |
0.00 |
21.37 |
0.75 |
0.86 |
| 8 |
Eg |
1509 |
1444 |
0.00 |
21.36 |
0.75 |
0.86 |
| 9 |
Eg |
1218 |
1165 |
0.00 |
0.84 |
0.75 |
0.86 |
| 9 |
Eg |
1218 |
1165 |
0.00 |
0.84 |
0.75 |
0.86 |
| 10 |
Eu |
3155 |
3019 |
63.07 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3155 |
3019 |
63.07 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1443 |
12.67 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1509 |
1443 |
12.67 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
824 |
788 |
4.90 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
824 |
788 |
4.90 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16503.0 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15786.8 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 B1B95/6-31+G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.761 |
| C2 |
0.000 |
0.000 |
-0.761 |
| H3 |
0.000 |
1.017 |
1.159 |
| H4 |
-0.881 |
-0.509 |
1.159 |
| H5 |
0.881 |
-0.509 |
1.159 |
| H6 |
0.000 |
-1.017 |
-1.159 |
| H7 |
-0.881 |
0.509 |
-1.159 |
| H8 |
0.881 |
0.509 |
-1.159 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5215 | 1.0924 | 1.0924 | 1.0924 | 2.1727 | 2.1727 | 2.1727 |
C2 | 1.5215 | | 2.1727 | 2.1727 | 2.1727 | 1.0924 | 1.0924 | 1.0924 | H3 | 1.0924 | 2.1727 | | 1.7618 | 1.7618 | 3.0844 | 2.5317 | 2.5317 | H4 | 1.0924 | 2.1727 | 1.7618 | | 1.7618 | 2.5317 | 2.5317 | 3.0844 | H5 | 1.0924 | 2.1727 | 1.7618 | 1.7618 | | 2.5317 | 3.0844 | 2.5317 | H6 | 2.1727 | 1.0924 | 3.0844 | 2.5317 | 2.5317 | | 1.7618 | 1.7618 | H7 | 2.1727 | 1.0924 | 2.5317 | 2.5317 | 3.0844 | 1.7618 | | 1.7618 | H8 | 2.1727 | 1.0924 | 2.5317 | 3.0844 | 2.5317 | 1.7618 | 1.7618 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.391 |
|
C1 |
C2 |
H7 |
111.391 |
| C1 |
C2 |
H8 |
111.391 |
|
C2 |
C1 |
H3 |
111.391 |
| C2 |
C1 |
H4 |
111.391 |
|
C2 |
C1 |
H5 |
111.391 |
| H3 |
C1 |
H4 |
107.485 |
|
H3 |
C1 |
H5 |
107.485 |
| H4 |
C1 |
H5 |
107.485 |
|
H6 |
C2 |
H7 |
107.485 |
| H6 |
C2 |
H8 |
107.485 |
|
H7 |
C2 |
H8 |
107.485 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.468 |
|
|
|
| 2 |
C |
-0.468 |
|
|
|
| 3 |
H |
0.156 |
|
|
|
| 4 |
H |
0.156 |
|
|
|
| 5 |
H |
0.156 |
|
|
|
| 6 |
H |
0.156 |
|
|
|
| 7 |
H |
0.156 |
|
|
|
| 8 |
H |
0.156 |
|
|
|
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 |
-14.891 |
0.000 |
0.000 |
| y |
0.000 |
-14.891 |
0.000 |
| z |
0.000 |
0.000 |
-15.543 |
|
| Traceless |
| | x | y | z |
| x |
0.326 |
0.000 |
0.000 |
| y |
0.000 |
0.326 |
0.000 |
| z |
0.000 |
0.000 |
-0.652 |
|
| Polar |
| 3z2-r2 | -1.303 |
| 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 |
3.597 |
0.000 |
0.000 |
| y |
0.000 |
3.597 |
0.000 |
| z |
0.000 |
0.000 |
3.978 |
<r2> (average value of r
2) Å
2
| <r2> |
30.651 |
| (<r2>)1/2 |
5.536 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -79.772586 |
| Energy at 298.15K | |
| HF Energy | -79.772586 |
| Nuclear repulsion energy | 42.139587 |
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 B1B95/6-31+G**
| 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' |
3083 |
2949 |
0.00 |
|
|
|
| 2 |
A1' |
1453 |
1390 |
0.00 |
|
|
|
| 3 |
A1' |
1025 |
981 |
0.00 |
|
|
|
| 4 |
A1" |
303i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3075 |
2941 |
69.40 |
|
|
|
| 6 |
A2" |
1403 |
1342 |
2.07 |
|
|
|
| 7 |
E' |
3162 |
3025 |
52.22 |
|
|
|
| 7 |
E' |
3162 |
3025 |
52.22 |
|
|
|
| 8 |
E' |
1516 |
1450 |
14.85 |
|
|
|
| 8 |
E' |
1516 |
1450 |
14.85 |
|
|
|
| 9 |
E' |
902 |
863 |
4.40 |
|
|
|
| 9 |
E' |
902 |
863 |
4.40 |
|
|
|
| 10 |
E" |
3141 |
3005 |
0.00 |
|
|
|
| 10 |
E" |
3141 |
3005 |
0.00 |
|
|
|
| 11 |
E" |
1506 |
1441 |
0.00 |
|
|
|
| 11 |
E" |
1506 |
1441 |
0.00 |
|
|
|
| 12 |
E" |
1168 |
1118 |
0.00 |
|
|
|
| 12 |
E" |
1168 |
1118 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16263.9 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 15558.1 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 B1B95/6-31+G**
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 |
1.013 |
1.174 |
| H4 |
-0.877 |
-0.506 |
1.174 |
| H5 |
0.877 |
-0.506 |
1.174 |
| H6 |
0.000 |
1.013 |
-1.174 |
| H7 |
0.877 |
-0.506 |
-1.174 |
| H8 |
-0.877 |
-0.506 |
-1.174 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5344 | 1.0914 | 1.0914 | 1.0914 | 2.1896 | 2.1896 | 2.1896 |
C2 | 1.5344 | | 2.1896 | 2.1896 | 2.1896 | 1.0914 | 1.0914 | 1.0914 | H3 | 1.0914 | 2.1896 | | 1.7542 | 1.7542 | 2.3482 | 2.9310 | 2.9310 | H4 | 1.0914 | 2.1896 | 1.7542 | | 1.7542 | 2.9310 | 2.9310 | 2.3482 | H5 | 1.0914 | 2.1896 | 1.7542 | 1.7542 | | 2.9310 | 2.3482 | 2.9310 | H6 | 2.1896 | 1.0914 | 2.3482 | 2.9310 | 2.9310 | | 1.7542 | 1.7542 | H7 | 2.1896 | 1.0914 | 2.9310 | 2.9310 | 2.3482 | 1.7542 | | 1.7542 | H8 | 2.1896 | 1.0914 | 2.9310 | 2.3482 | 2.9310 | 1.7542 | 1.7542 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.888 |
|
C1 |
C2 |
H7 |
111.888 |
| C1 |
C2 |
H8 |
111.888 |
|
C2 |
C1 |
H3 |
111.888 |
| C2 |
C1 |
H4 |
111.888 |
|
C2 |
C1 |
H5 |
111.888 |
| H3 |
C1 |
H4 |
106.950 |
|
H3 |
C1 |
H5 |
106.950 |
| H4 |
C1 |
H5 |
106.950 |
|
H6 |
C2 |
H7 |
106.950 |
| H6 |
C2 |
H8 |
106.950 |
|
H7 |
C2 |
H8 |
106.950 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.477 |
|
|
|
| 2 |
C |
-0.477 |
|
|
|
| 3 |
H |
0.159 |
|
|
|
| 4 |
H |
0.159 |
|
|
|
| 5 |
H |
0.159 |
|
|
|
| 6 |
H |
0.159 |
|
|
|
| 7 |
H |
0.159 |
|
|
|
| 8 |
H |
0.159 |
|
|
|
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 |
-14.886 |
0.000 |
0.000 |
| y |
0.000 |
-14.886 |
0.000 |
| z |
0.000 |
0.000 |
-15.510 |
|
| Traceless |
| | x | y | z |
| x |
0.312 |
0.000 |
0.000 |
| y |
0.000 |
0.312 |
0.000 |
| z |
0.000 |
0.000 |
-0.624 |
|
| Polar |
| 3z2-r2 | -1.248 |
| 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 |
3.547 |
0.000 |
0.000 |
| y |
0.000 |
3.547 |
0.000 |
| z |
0.000 |
0.000 |
3.888 |
<r2> (average value of r
2) Å
2
| <r2> |
30.916 |
| (<r2>)1/2 |
5.560 |