Jump to
S1C2
Energy calculated at B3PW91/TZVP
| | hartrees |
| Energy at 0K | -79.831037 |
| Energy at 298.15K | -79.836948 |
| HF Energy | -79.831037 |
| Nuclear repulsion energy | 42.271100 |
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 B3PW91/TZVP
| 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 |
3039 |
2930 |
0.00 |
289.93 |
0.01 |
0.01 |
| 2 |
A1g |
1424 |
1374 |
0.00 |
2.64 |
0.73 |
0.84 |
| 3 |
A1g |
1012 |
976 |
0.00 |
10.79 |
0.25 |
0.40 |
| 4 |
A1u |
310 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3039 |
2931 |
59.31 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1404 |
1354 |
2.56 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3094 |
2984 |
0.00 |
141.89 |
0.75 |
0.86 |
| 7 |
Eg |
3094 |
2984 |
0.00 |
141.89 |
0.75 |
0.86 |
| 8 |
Eg |
1501 |
1447 |
0.00 |
26.55 |
0.75 |
0.86 |
| 8 |
Eg |
1501 |
1447 |
0.00 |
26.55 |
0.75 |
0.86 |
| 9 |
Eg |
1217 |
1174 |
0.00 |
0.62 |
0.75 |
0.86 |
| 9 |
Eg |
1217 |
1174 |
0.00 |
0.62 |
0.75 |
0.86 |
| 10 |
Eu |
3119 |
3008 |
63.61 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3119 |
3008 |
63.61 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1502 |
1448 |
12.01 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1502 |
1448 |
12.01 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
797 |
4.75 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
827 |
797 |
4.75 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16373.3 cm
-1
Scaled (by 0.9643) Zero Point Vibrational Energy (zpe) 15788.8 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 B3PW91/TZVP
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 |
1.160 |
| H4 |
-0.881 |
-0.509 |
1.160 |
| H5 |
0.881 |
-0.509 |
1.160 |
| H6 |
0.000 |
-1.017 |
-1.160 |
| H7 |
-0.881 |
0.509 |
-1.160 |
| H8 |
0.881 |
0.509 |
-1.160 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5228 | 1.0929 | 1.0929 | 1.0929 | 2.1745 | 2.1745 | 2.1745 |
C2 | 1.5228 | | 2.1745 | 2.1745 | 2.1745 | 1.0929 | 1.0929 | 1.0929 | H3 | 1.0929 | 2.1745 | | 1.7623 | 1.7623 | 3.0866 | 2.5341 | 2.5341 | H4 | 1.0929 | 2.1745 | 1.7623 | | 1.7623 | 2.5341 | 2.5341 | 3.0866 | H5 | 1.0929 | 2.1745 | 1.7623 | 1.7623 | | 2.5341 | 3.0866 | 2.5341 | H6 | 2.1745 | 1.0929 | 3.0866 | 2.5341 | 2.5341 | | 1.7623 | 1.7623 | H7 | 2.1745 | 1.0929 | 2.5341 | 2.5341 | 3.0866 | 1.7623 | | 1.7623 | H8 | 2.1745 | 1.0929 | 2.5341 | 3.0866 | 2.5341 | 1.7623 | 1.7623 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.415 |
|
C1 |
C2 |
H7 |
111.415 |
| C1 |
C2 |
H8 |
111.415 |
|
C2 |
C1 |
H3 |
111.415 |
| C2 |
C1 |
H4 |
111.415 |
|
C2 |
C1 |
H5 |
111.415 |
| H3 |
C1 |
H4 |
107.460 |
|
H3 |
C1 |
H5 |
107.460 |
| H4 |
C1 |
H5 |
107.460 |
|
H6 |
C2 |
H7 |
107.460 |
| H6 |
C2 |
H8 |
107.460 |
|
H7 |
C2 |
H8 |
107.460 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.347 |
|
|
|
| 2 |
C |
-0.347 |
|
|
|
| 3 |
H |
0.116 |
|
|
|
| 4 |
H |
0.116 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.116 |
|
|
|
| 7 |
H |
0.116 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
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 |
-14.842 |
0.000 |
0.000 |
| y |
0.000 |
-14.842 |
0.000 |
| z |
0.000 |
0.000 |
-15.509 |
|
| Traceless |
| | x | y | z |
| x |
0.333 |
0.000 |
0.000 |
| y |
0.000 |
0.333 |
0.000 |
| z |
0.000 |
0.000 |
-0.667 |
|
| Polar |
| 3z2-r2 | -1.333 |
| 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 |
3.770 |
0.000 |
0.000 |
| y |
0.000 |
3.770 |
0.000 |
| z |
0.000 |
0.000 |
4.117 |
<r2> (average value of r
2) Å
2
| <r2> |
30.656 |
| (<r2>)1/2 |
5.537 |
Jump to
S1C1
Energy calculated at B3PW91/TZVP
| | hartrees |
| Energy at 0K | -79.826691 |
| Energy at 298.15K | |
| HF Energy | -79.826691 |
| Nuclear repulsion energy | 42.111986 |
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 B3PW91/TZVP
| 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' |
3054 |
2945 |
0.00 |
|
|
|
| 2 |
A1' |
1441 |
1390 |
0.00 |
|
|
|
| 3 |
A1' |
1009 |
973 |
0.00 |
|
|
|
| 4 |
A1" |
300i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3048 |
2939 |
63.69 |
|
|
|
| 6 |
A2" |
1402 |
1352 |
2.99 |
|
|
|
| 7 |
E' |
3126 |
3015 |
52.26 |
|
|
|
| 7 |
E' |
3126 |
3015 |
52.26 |
|
|
|
| 8 |
E' |
1508 |
1454 |
14.56 |
|
|
|
| 8 |
E' |
1508 |
1454 |
14.56 |
|
|
|
| 9 |
E' |
898 |
866 |
4.37 |
|
|
|
| 9 |
E' |
898 |
866 |
4.37 |
|
|
|
| 10 |
E" |
3104 |
2994 |
0.00 |
|
|
|
| 10 |
E" |
3104 |
2994 |
0.00 |
|
|
|
| 11 |
E" |
1498 |
1445 |
0.00 |
|
|
|
| 11 |
E" |
1498 |
1445 |
0.00 |
|
|
|
| 12 |
E" |
1167 |
1125 |
0.00 |
|
|
|
| 12 |
E" |
1167 |
1125 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16128.4 cm
-1
Scaled (by 0.9643) Zero Point Vibrational Energy (zpe) 15552.6 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 B3PW91/TZVP
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.768 |
| C2 |
0.000 |
0.000 |
-0.768 |
| H3 |
0.000 |
1.013 |
1.175 |
| H4 |
-0.877 |
-0.507 |
1.175 |
| H5 |
0.877 |
-0.507 |
1.175 |
| H6 |
0.000 |
1.013 |
-1.175 |
| H7 |
0.877 |
-0.507 |
-1.175 |
| H8 |
-0.877 |
-0.507 |
-1.175 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5361 | 1.0918 | 1.0918 | 1.0918 | 2.1912 | 2.1912 | 2.1912 |
C2 | 1.5361 | | 2.1912 | 2.1912 | 2.1912 | 1.0918 | 1.0918 | 1.0918 | H3 | 1.0918 | 2.1912 | | 1.7548 | 1.7548 | 2.3498 | 2.9328 | 2.9328 | H4 | 1.0918 | 2.1912 | 1.7548 | | 1.7548 | 2.9328 | 2.9328 | 2.3498 | H5 | 1.0918 | 2.1912 | 1.7548 | 1.7548 | | 2.9328 | 2.3498 | 2.9328 | H6 | 2.1912 | 1.0918 | 2.3498 | 2.9328 | 2.9328 | | 1.7548 | 1.7548 | H7 | 2.1912 | 1.0918 | 2.9328 | 2.9328 | 2.3498 | 1.7548 | | 1.7548 | H8 | 2.1912 | 1.0918 | 2.9328 | 2.3498 | 2.9328 | 1.7548 | 1.7548 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.880 |
|
C1 |
C2 |
H7 |
111.880 |
| C1 |
C2 |
H8 |
111.880 |
|
C2 |
C1 |
H3 |
111.880 |
| C2 |
C1 |
H4 |
111.880 |
|
C2 |
C1 |
H5 |
111.880 |
| H3 |
C1 |
H4 |
106.959 |
|
H3 |
C1 |
H5 |
106.959 |
| H4 |
C1 |
H5 |
106.959 |
|
H6 |
C2 |
H7 |
106.959 |
| H6 |
C2 |
H8 |
106.959 |
|
H7 |
C2 |
H8 |
106.959 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.366 |
|
|
|
| 2 |
C |
-0.366 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.122 |
|
|
|
| 6 |
H |
0.122 |
|
|
|
| 7 |
H |
0.122 |
|
|
|
| 8 |
H |
0.122 |
|
|
|
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 |
-14.829 |
0.000 |
0.000 |
| y |
0.000 |
-14.829 |
0.000 |
| z |
0.000 |
0.000 |
-15.492 |
|
| Traceless |
| | x | y | z |
| x |
0.332 |
0.000 |
0.000 |
| y |
0.000 |
0.332 |
0.000 |
| z |
0.000 |
0.000 |
-0.664 |
|
| Polar |
| 3z2-r2 | -1.328 |
| 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 |
3.731 |
0.000 |
0.000 |
| y |
0.000 |
3.731 |
0.000 |
| z |
0.000 |
0.000 |
3.930 |
<r2> (average value of r
2) Å
2
| <r2> |
30.920 |
| (<r2>)1/2 |
5.561 |