Jump to
S1C2
Energy calculated at B97D3/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.810981 |
| Energy at 298.15K | -79.816855 |
| HF Energy | -79.810981 |
| Nuclear repulsion energy | 42.128847 |
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 B97D3/aug-cc-pVTZ
| 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 |
2977 |
2932 |
0.00 |
369.09 |
0.00 |
0.01 |
| 2 |
A1g |
1390 |
1369 |
0.00 |
0.06 |
0.03 |
0.05 |
| 3 |
A1g |
976 |
961 |
0.00 |
11.75 |
0.18 |
0.30 |
| 4 |
A1u |
299 |
294 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
2979 |
2933 |
69.89 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1381 |
1360 |
0.33 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3026 |
2980 |
0.00 |
134.10 |
0.75 |
0.86 |
| 7 |
Eg |
3026 |
2980 |
0.00 |
133.87 |
0.75 |
0.86 |
| 8 |
Eg |
1474 |
1451 |
0.00 |
8.52 |
0.75 |
0.86 |
| 8 |
Eg |
1474 |
1451 |
0.00 |
8.55 |
0.75 |
0.86 |
| 9 |
Eg |
1197 |
1179 |
0.00 |
0.12 |
0.75 |
0.86 |
| 9 |
Eg |
1197 |
1179 |
0.00 |
0.12 |
0.75 |
0.86 |
| 10 |
Eu |
3052 |
3005 |
73.42 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3052 |
3005 |
73.42 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1476 |
1454 |
7.78 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1476 |
1454 |
7.78 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
812 |
799 |
3.49 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
812 |
799 |
3.49 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16038.0 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 15792.6 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 B97D3/aug-cc-pVTZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.765 |
| C2 |
0.000 |
0.000 |
-0.765 |
| H3 |
0.000 |
1.020 |
1.164 |
| H4 |
-0.884 |
-0.510 |
1.164 |
| H5 |
0.884 |
-0.510 |
1.164 |
| H6 |
0.000 |
-1.020 |
-1.164 |
| H7 |
-0.884 |
0.510 |
-1.164 |
| H8 |
0.884 |
0.510 |
-1.164 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5304 | 1.0954 | 1.0954 | 1.0954 | 2.1821 | 2.1821 | 2.1821 |
C2 | 1.5304 | | 2.1821 | 2.1821 | 2.1821 | 1.0954 | 1.0954 | 1.0954 | H3 | 1.0954 | 2.1821 | | 1.7673 | 1.7673 | 3.0952 | 2.5411 | 2.5411 | H4 | 1.0954 | 2.1821 | 1.7673 | | 1.7673 | 2.5411 | 2.5411 | 3.0952 | H5 | 1.0954 | 2.1821 | 1.7673 | 1.7673 | | 2.5411 | 3.0952 | 2.5411 | H6 | 2.1821 | 1.0954 | 3.0952 | 2.5411 | 2.5411 | | 1.7673 | 1.7673 | H7 | 2.1821 | 1.0954 | 2.5411 | 2.5411 | 3.0952 | 1.7673 | | 1.7673 | H8 | 2.1821 | 1.0954 | 2.5411 | 3.0952 | 2.5411 | 1.7673 | 1.7673 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.329 |
|
C1 |
C2 |
H7 |
111.329 |
| C1 |
C2 |
H8 |
111.329 |
|
C2 |
C1 |
H3 |
111.329 |
| C2 |
C1 |
H4 |
111.329 |
|
C2 |
C1 |
H5 |
111.329 |
| H3 |
C1 |
H4 |
107.551 |
|
H3 |
C1 |
H5 |
107.551 |
| H4 |
C1 |
H5 |
107.551 |
|
H6 |
C2 |
H7 |
107.551 |
| H6 |
C2 |
H8 |
107.551 |
|
H7 |
C2 |
H8 |
107.551 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.443 |
|
|
|
| 2 |
C |
-0.443 |
|
|
|
| 3 |
H |
0.148 |
|
|
|
| 4 |
H |
0.148 |
|
|
|
| 5 |
H |
0.148 |
|
|
|
| 6 |
H |
0.148 |
|
|
|
| 7 |
H |
0.148 |
|
|
|
| 8 |
H |
0.148 |
|
|
|
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 |
-14.976 |
0.000 |
0.000 |
| y |
0.000 |
-14.976 |
0.000 |
| z |
0.000 |
0.000 |
-15.705 |
|
| Traceless |
| | x | y | z |
| x |
0.365 |
0.000 |
0.000 |
| y |
0.000 |
0.365 |
0.000 |
| z |
0.000 |
0.000 |
-0.729 |
|
| Polar |
| 3z2-r2 | -1.458 |
| 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 |
4.211 |
0.000 |
0.000 |
| y |
0.000 |
4.211 |
0.000 |
| z |
0.000 |
0.000 |
4.856 |
<r2> (average value of r
2) Å
2
| <r2> |
30.903 |
| (<r2>)1/2 |
5.559 |
Jump to
S1C1
Energy calculated at B97D3/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -79.806888 |
| Energy at 298.15K | |
| HF Energy | -79.806888 |
| Nuclear repulsion energy | 41.961083 |
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 B97D3/aug-cc-pVTZ
| 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' |
2991 |
2946 |
0.00 |
|
|
|
| 2 |
A1' |
1407 |
1386 |
0.00 |
|
|
|
| 3 |
A1' |
970 |
955 |
0.00 |
|
|
|
| 4 |
A1" |
296i |
291i |
0.00 |
|
|
|
| 5 |
A2" |
2985 |
2939 |
71.35 |
|
|
|
| 6 |
A2" |
1377 |
1356 |
0.14 |
|
|
|
| 7 |
E' |
3059 |
3012 |
62.09 |
|
|
|
| 7 |
E' |
3059 |
3012 |
62.08 |
|
|
|
| 8 |
E' |
1480 |
1457 |
9.23 |
|
|
|
| 8 |
E' |
1480 |
1457 |
9.23 |
|
|
|
| 9 |
E' |
884 |
870 |
2.48 |
|
|
|
| 9 |
E' |
884 |
870 |
2.48 |
|
|
|
| 10 |
E" |
3036 |
2989 |
0.00 |
|
|
|
| 10 |
E" |
3036 |
2989 |
0.00 |
|
|
|
| 11 |
E" |
1473 |
1451 |
0.00 |
|
|
|
| 11 |
E" |
1473 |
1451 |
0.00 |
|
|
|
| 12 |
E" |
1148 |
1130 |
0.00 |
|
|
|
| 12 |
E" |
1148 |
1130 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15795.8 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 15554.1 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 B97D3/aug-cc-pVTZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.772 |
| C2 |
0.000 |
0.000 |
-0.772 |
| H3 |
0.000 |
1.016 |
1.178 |
| H4 |
-0.880 |
-0.508 |
1.178 |
| H5 |
0.880 |
-0.508 |
1.178 |
| H6 |
0.000 |
1.016 |
-1.178 |
| H7 |
0.880 |
-0.508 |
-1.178 |
| H8 |
-0.880 |
-0.508 |
-1.178 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5450 | 1.0942 | 1.0942 | 1.0942 | 2.1991 | 2.1991 | 2.1991 |
C2 | 1.5450 | | 2.1991 | 2.1991 | 2.1991 | 1.0942 | 1.0942 | 1.0942 | H3 | 1.0942 | 2.1991 | | 1.7605 | 1.7605 | 2.3553 | 2.9406 | 2.9406 | H4 | 1.0942 | 2.1991 | 1.7605 | | 1.7605 | 2.9406 | 2.9406 | 2.3553 | H5 | 1.0942 | 2.1991 | 1.7605 | 1.7605 | | 2.9406 | 2.3553 | 2.9406 | H6 | 2.1991 | 1.0942 | 2.3553 | 2.9406 | 2.9406 | | 1.7605 | 1.7605 | H7 | 2.1991 | 1.0942 | 2.9406 | 2.9406 | 2.3553 | 1.7605 | | 1.7605 | H8 | 2.1991 | 1.0942 | 2.9406 | 2.3553 | 2.9406 | 1.7605 | 1.7605 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.734 |
|
C1 |
C2 |
H7 |
111.734 |
| C1 |
C2 |
H8 |
111.734 |
|
C2 |
C1 |
H3 |
111.734 |
| C2 |
C1 |
H4 |
111.734 |
|
C2 |
C1 |
H5 |
111.734 |
| H3 |
C1 |
H4 |
107.116 |
|
H3 |
C1 |
H5 |
107.116 |
| H4 |
C1 |
H5 |
107.116 |
|
H6 |
C2 |
H7 |
107.116 |
| H6 |
C2 |
H8 |
107.116 |
|
H7 |
C2 |
H8 |
107.116 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.451 |
|
|
|
| 2 |
C |
-0.451 |
|
|
|
| 3 |
H |
0.150 |
|
|
|
| 4 |
H |
0.150 |
|
|
|
| 5 |
H |
0.150 |
|
|
|
| 6 |
H |
0.150 |
|
|
|
| 7 |
H |
0.150 |
|
|
|
| 8 |
H |
0.150 |
|
|
|
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 |
-14.961 |
0.000 |
0.000 |
| y |
0.000 |
-14.961 |
0.000 |
| z |
0.000 |
0.000 |
-15.694 |
|
| Traceless |
| | x | y | z |
| x |
0.366 |
0.000 |
0.000 |
| y |
0.000 |
0.366 |
0.000 |
| z |
0.000 |
0.000 |
-0.733 |
|
| Polar |
| 3z2-r2 | -1.465 |
| 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 |
4.173 |
0.000 |
0.000 |
| y |
0.000 |
4.173 |
0.000 |
| z |
0.000 |
0.000 |
4.868 |
<r2> (average value of r
2) Å
2
| <r2> |
31.178 |
| (<r2>)1/2 |
5.584 |