Jump to
S1C2
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.844068 |
| Energy at 298.15K | -79.849968 |
| HF Energy | -79.844068 |
| Nuclear repulsion energy | 42.133623 |
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 TPSSh/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 |
3034 |
2928 |
0.00 |
220.74 |
0.01 |
0.02 |
| 2 |
A1g |
1428 |
1378 |
0.00 |
5.27 |
0.72 |
0.83 |
| 3 |
A1g |
1004 |
968 |
0.00 |
9.75 |
0.26 |
0.42 |
| 4 |
A1u |
310 |
299 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3034 |
2927 |
61.58 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1411 |
1362 |
0.02 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3088 |
2980 |
0.00 |
134.12 |
0.75 |
0.86 |
| 7 |
Eg |
3088 |
2980 |
0.00 |
134.12 |
0.75 |
0.86 |
| 8 |
Eg |
1515 |
1462 |
0.00 |
31.19 |
0.75 |
0.86 |
| 8 |
Eg |
1515 |
1462 |
0.00 |
31.19 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1183 |
0.00 |
2.03 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1183 |
0.00 |
2.03 |
0.75 |
0.86 |
| 10 |
Eu |
3114 |
3005 |
71.87 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3114 |
3005 |
71.89 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1520 |
1467 |
5.01 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1520 |
1467 |
5.00 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
815 |
787 |
3.66 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
815 |
787 |
3.66 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16387.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15814.3 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 TPSSh/6-31G(2df,p)
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 |
1.021 |
1.163 |
| H4 |
-0.884 |
-0.510 |
1.163 |
| H5 |
0.884 |
-0.510 |
1.163 |
| H6 |
0.000 |
-1.021 |
-1.163 |
| H7 |
-0.884 |
0.510 |
-1.163 |
| H8 |
0.884 |
0.510 |
-1.163 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5309 | 1.0951 | 1.0951 | 1.0951 | 2.1814 | 2.1814 | 2.1814 |
C2 | 1.5309 | | 2.1814 | 2.1814 | 2.1814 | 1.0951 | 1.0951 | 1.0951 | H3 | 1.0951 | 2.1814 | | 1.7676 | 1.7676 | 3.0938 | 2.5391 | 2.5391 | H4 | 1.0951 | 2.1814 | 1.7676 | | 1.7676 | 2.5391 | 2.5391 | 3.0938 | H5 | 1.0951 | 2.1814 | 1.7676 | 1.7676 | | 2.5391 | 3.0938 | 2.5391 | H6 | 2.1814 | 1.0951 | 3.0938 | 2.5391 | 2.5391 | | 1.7676 | 1.7676 | H7 | 2.1814 | 1.0951 | 2.5391 | 2.5391 | 3.0938 | 1.7676 | | 1.7676 | H8 | 2.1814 | 1.0951 | 2.5391 | 3.0938 | 2.5391 | 1.7676 | 1.7676 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.261 |
|
C1 |
C2 |
H7 |
111.261 |
| C1 |
C2 |
H8 |
111.261 |
|
C2 |
C1 |
H3 |
111.261 |
| C2 |
C1 |
H4 |
111.261 |
|
C2 |
C1 |
H5 |
111.261 |
| H3 |
C1 |
H4 |
107.624 |
|
H3 |
C1 |
H5 |
107.624 |
| H4 |
C1 |
H5 |
107.624 |
|
H6 |
C2 |
H7 |
107.624 |
| H6 |
C2 |
H8 |
107.624 |
|
H7 |
C2 |
H8 |
107.624 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.404 |
|
|
|
| 2 |
C |
-0.404 |
|
|
|
| 3 |
H |
0.135 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
| 5 |
H |
0.135 |
|
|
|
| 6 |
H |
0.135 |
|
|
|
| 7 |
H |
0.135 |
|
|
|
| 8 |
H |
0.135 |
|
|
|
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.466 |
0.000 |
0.000 |
| y |
0.000 |
3.466 |
0.000 |
| z |
0.000 |
0.000 |
3.804 |
<r2> (average value of r
2) Å
2
| <r2> |
30.612 |
| (<r2>)1/2 |
5.533 |
Jump to
S1C1
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -79.839681 |
| Energy at 298.15K | |
| HF Energy | -79.839681 |
| Nuclear repulsion energy | 41.963935 |
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 TPSSh/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' |
3048 |
2941 |
0.00 |
|
|
|
| 2 |
A1' |
1446 |
1395 |
0.00 |
|
|
|
| 3 |
A1' |
999 |
964 |
0.00 |
|
|
|
| 4 |
A1" |
302i |
292i |
0.00 |
|
|
|
| 5 |
A2" |
3040 |
2933 |
62.44 |
|
|
|
| 6 |
A2" |
1408 |
1358 |
0.13 |
|
|
|
| 7 |
E' |
3120 |
3011 |
60.49 |
|
|
|
| 7 |
E' |
3120 |
3011 |
60.49 |
|
|
|
| 8 |
E' |
1523 |
1470 |
6.12 |
|
|
|
| 8 |
E' |
1523 |
1470 |
6.11 |
|
|
|
| 9 |
E' |
891 |
860 |
2.76 |
|
|
|
| 9 |
E' |
891 |
860 |
2.76 |
|
|
|
| 10 |
E" |
3098 |
2989 |
0.00 |
|
|
|
| 10 |
E" |
3098 |
2989 |
0.00 |
|
|
|
| 11 |
E" |
1516 |
1463 |
0.00 |
|
|
|
| 11 |
E" |
1516 |
1463 |
0.00 |
|
|
|
| 12 |
E" |
1176 |
1135 |
0.00 |
|
|
|
| 12 |
E" |
1176 |
1135 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16141.9 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 15576.9 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 TPSSh/6-31G(2df,p)
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.773 |
| C2 |
0.000 |
0.000 |
-0.773 |
| H3 |
0.000 |
1.017 |
1.177 |
| H4 |
-0.880 |
-0.508 |
1.177 |
| H5 |
0.880 |
-0.508 |
1.177 |
| H6 |
0.000 |
1.017 |
-1.177 |
| H7 |
0.880 |
-0.508 |
-1.177 |
| H8 |
-0.880 |
-0.508 |
-1.177 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5463 | 1.0939 | 1.0939 | 1.0939 | 2.1994 | 2.1994 | 2.1994 |
C2 | 1.5463 | | 2.1994 | 2.1994 | 2.1994 | 1.0939 | 1.0939 | 1.0939 | H3 | 1.0939 | 2.1994 | | 1.7607 | 1.7607 | 2.3543 | 2.9399 | 2.9399 | H4 | 1.0939 | 2.1994 | 1.7607 | | 1.7607 | 2.9399 | 2.9399 | 2.3543 | H5 | 1.0939 | 2.1994 | 1.7607 | 1.7607 | | 2.9399 | 2.3543 | 2.9399 | H6 | 2.1994 | 1.0939 | 2.3543 | 2.9399 | 2.9399 | | 1.7607 | 1.7607 | H7 | 2.1994 | 1.0939 | 2.9399 | 2.9399 | 2.3543 | 1.7607 | | 1.7607 | H8 | 2.1994 | 1.0939 | 2.9399 | 2.3543 | 2.9399 | 1.7607 | 1.7607 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.674 |
|
C1 |
C2 |
H7 |
111.674 |
| C1 |
C2 |
H8 |
111.674 |
|
C2 |
C1 |
H3 |
111.674 |
| C2 |
C1 |
H4 |
111.674 |
|
C2 |
C1 |
H5 |
111.674 |
| H3 |
C1 |
H4 |
107.181 |
|
H3 |
C1 |
H5 |
107.181 |
| H4 |
C1 |
H5 |
107.181 |
|
H6 |
C2 |
H7 |
107.181 |
| H6 |
C2 |
H8 |
107.181 |
|
H7 |
C2 |
H8 |
107.181 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability