Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -117.140148 |
| Energy at 298.15K | -117.144395 |
| HF Energy | -117.140148 |
| Nuclear repulsion energy | 65.015781 |
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 HSEh1PBE/6-311G*
| 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 |
3263 |
3131 |
23.45 |
|
|
|
| 2 |
A1 |
3165 |
3037 |
1.17 |
|
|
|
| 3 |
A1 |
3158 |
3030 |
21.07 |
|
|
|
| 4 |
A1 |
1527 |
1465 |
3.39 |
|
|
|
| 5 |
A1 |
1282 |
1230 |
1.06 |
|
|
|
| 6 |
A1 |
1045 |
1003 |
0.18 |
|
|
|
| 7 |
A1 |
427 |
409 |
0.02 |
|
|
|
| 8 |
A2 |
772 |
741 |
0.00 |
|
|
|
| 9 |
A2 |
554 |
531 |
0.00 |
|
|
|
| 10 |
B1 |
1007 |
967 |
24.64 |
|
|
|
| 11 |
B1 |
798 |
766 |
88.22 |
|
|
|
| 12 |
B1 |
530 |
509 |
20.30 |
|
|
|
| 13 |
B2 |
3260 |
3128 |
6.79 |
|
|
|
| 14 |
B2 |
3158 |
3030 |
12.60 |
|
|
|
| 15 |
B2 |
1525 |
1464 |
0.53 |
|
|
|
| 16 |
B2 |
1427 |
1369 |
8.62 |
|
|
|
| 17 |
B2 |
1215 |
1166 |
0.03 |
|
|
|
| 18 |
B2 |
939 |
901 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14525.6 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 13938.8 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 HSEh1PBE/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.442 |
| H2 |
0.000 |
0.000 |
1.532 |
| C3 |
0.000 |
1.224 |
-0.196 |
| C4 |
0.000 |
-1.224 |
-0.196 |
| H5 |
0.000 |
2.154 |
0.360 |
| H6 |
0.000 |
-2.154 |
0.360 |
| H7 |
0.000 |
1.292 |
-1.279 |
| H8 |
0.000 |
-1.292 |
-1.279 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0892 | 1.3807 | 1.3807 | 2.1559 | 2.1559 | 2.1526 | 2.1526 |
H2 | 1.0892 | | 2.1173 | 2.1173 | 2.4522 | 2.4522 | 3.0937 | 3.0937 | C3 | 1.3807 | 2.1173 | | 2.4488 | 1.0835 | 3.4241 | 1.0857 | 2.7397 | C4 | 1.3807 | 2.1173 | 2.4488 | | 3.4241 | 1.0835 | 2.7397 | 1.0857 | H5 | 2.1559 | 2.4522 | 1.0835 | 3.4241 | | 4.3086 | 1.8526 | 3.8163 | H6 | 2.1559 | 2.4522 | 3.4241 | 1.0835 | 4.3086 | | 3.8163 | 1.8526 | H7 | 2.1526 | 3.0937 | 1.0857 | 2.7397 | 1.8526 | 3.8163 | | 2.5838 | H8 | 2.1526 | 3.0937 | 2.7397 | 1.0857 | 3.8163 | 1.8526 | 2.5838 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.591 |
|
C1 |
C3 |
H7 |
121.095 |
| C1 |
C4 |
H6 |
121.591 |
|
C1 |
C4 |
H8 |
121.095 |
| H2 |
C1 |
C3 |
117.531 |
|
H2 |
C1 |
C4 |
117.531 |
| C3 |
C1 |
C4 |
124.938 |
|
H5 |
C3 |
H7 |
117.314 |
| H6 |
C4 |
H8 |
117.314 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.197 |
|
|
|
| 2 |
H |
0.203 |
|
|
|
| 3 |
C |
-0.447 |
|
|
|
| 4 |
C |
-0.447 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
| 6 |
H |
0.224 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
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 |
0.063 |
0.063 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.312 |
0.000 |
0.000 |
| y |
0.000 |
-17.623 |
0.000 |
| z |
0.000 |
0.000 |
-17.403 |
|
| Traceless |
| | x | y | z |
| x |
-4.799 |
0.000 |
0.000 |
| y |
0.000 |
2.235 |
0.000 |
| z |
0.000 |
0.000 |
2.564 |
|
| Polar |
| 3z2-r2 | 5.128 |
| x2-y2 | -4.689 |
| 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 |
2.501 |
0.000 |
0.000 |
| y |
0.000 |
7.702 |
0.000 |
| z |
0.000 |
0.000 |
4.720 |
<r2> (average value of r
2) Å
2
| <r2> |
50.060 |
| (<r2>)1/2 |
7.075 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -117.140148 |
| Energy at 298.15K | -117.144396 |
| HF Energy | -117.140148 |
| Nuclear repulsion energy | 65.017203 |
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 HSEh1PBE/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3262 |
3130 |
23.31 |
|
|
|
| 2 |
A' |
3259 |
3128 |
6.97 |
|
|
|
| 3 |
A' |
3165 |
3037 |
1.07 |
|
|
|
| 4 |
A' |
3158 |
3030 |
19.65 |
|
|
|
| 5 |
A' |
3157 |
3030 |
14.11 |
|
|
|
| 6 |
A' |
1527 |
1465 |
3.40 |
|
|
|
| 7 |
A' |
1526 |
1464 |
0.53 |
|
|
|
| 8 |
A' |
1427 |
1369 |
8.62 |
|
|
|
| 9 |
A' |
1282 |
1230 |
1.06 |
|
|
|
| 10 |
A' |
1215 |
1166 |
0.03 |
|
|
|
| 11 |
A' |
1046 |
1003 |
0.19 |
|
|
|
| 12 |
A' |
939 |
902 |
0.13 |
|
|
|
| 13 |
A' |
427 |
410 |
0.02 |
|
|
|
| 14 |
A" |
1007 |
967 |
24.64 |
|
|
|
| 15 |
A" |
798 |
766 |
88.25 |
|
|
|
| 16 |
A" |
772 |
741 |
0.00 |
|
|
|
| 17 |
A" |
554 |
532 |
0.00 |
|
|
|
| 18 |
A" |
531 |
509 |
20.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14525.8 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 13939.0 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.443 |
0.000 |
| H2 |
0.000 |
1.532 |
0.000 |
| C3 |
-1.224 |
-0.196 |
0.000 |
| C4 |
1.224 |
-0.196 |
0.000 |
| H5 |
-2.155 |
0.360 |
0.000 |
| H6 |
2.154 |
0.360 |
0.000 |
| H7 |
-1.291 |
-1.279 |
0.000 |
| H8 |
1.292 |
-1.279 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0892 | 1.3807 | 1.3807 | 2.1561 | 2.1559 | 2.1524 | 2.1526 |
H2 | 1.0892 | | 2.1175 | 2.1172 | 2.4528 | 2.4522 | 3.0937 | 3.0936 | C3 | 1.3807 | 2.1175 | | 2.4486 | 1.0836 | 3.4240 | 1.0857 | 2.7394 | C4 | 1.3807 | 2.1172 | 2.4486 | | 3.4242 | 1.0835 | 2.7391 | 1.0857 | H5 | 2.1561 | 2.4528 | 1.0836 | 3.4242 | | 4.3088 | 1.8527 | 3.8163 | H6 | 2.1559 | 2.4522 | 3.4240 | 1.0835 | 4.3088 | | 3.8158 | 1.8525 | H7 | 2.1524 | 3.0937 | 1.0857 | 2.7391 | 1.8527 | 3.8158 | | 2.5831 | H8 | 2.1526 | 3.0936 | 2.7394 | 1.0857 | 3.8163 | 1.8525 | 2.5831 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.607 |
|
C1 |
C3 |
H7 |
121.081 |
| C1 |
C4 |
H6 |
121.602 |
|
C1 |
C4 |
H8 |
121.097 |
| H2 |
C1 |
C3 |
117.550 |
|
H2 |
C1 |
C4 |
117.524 |
| C3 |
C1 |
C4 |
124.926 |
|
H5 |
C3 |
H7 |
117.312 |
| H6 |
C4 |
H8 |
117.300 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.197 |
|
|
|
| 2 |
H |
0.203 |
|
|
|
| 3 |
C |
-0.447 |
|
|
|
| 4 |
C |
-0.447 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
| 6 |
H |
0.224 |
|
|
|
| 7 |
H |
0.219 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.063 |
0.000 |
0.063 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.623 |
0.000 |
0.000 |
| y |
0.000 |
-17.404 |
0.000 |
| z |
0.000 |
0.000 |
-22.312 |
|
| Traceless |
| | x | y | z |
| x |
2.235 |
0.000 |
0.000 |
| y |
0.000 |
2.564 |
0.000 |
| z |
0.000 |
0.000 |
-4.799 |
|
| Polar |
| 3z2-r2 | -9.598 |
| x2-y2 | -0.219 |
| 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 |
7.702 |
-0.000 |
0.000 |
| y |
-0.000 |
4.720 |
0.000 |
| z |
0.000 |
0.000 |
2.501 |
<r2> (average value of r
2) Å
2
| <r2> |
50.057 |
| (<r2>)1/2 |
7.075 |