Jump to
S1C2
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -117.125314 |
| Energy at 298.15K | -117.129561 |
| HF Energy | -117.125314 |
| Nuclear repulsion energy | 64.747220 |
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/cc-pVDZ
| 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 |
3280 |
3155 |
12.26 |
|
|
|
| 2 |
A1 |
3173 |
3052 |
0.29 |
|
|
|
| 3 |
A1 |
3166 |
3046 |
15.18 |
|
|
|
| 4 |
A1 |
1501 |
1443 |
2.35 |
|
|
|
| 5 |
A1 |
1268 |
1220 |
1.44 |
|
|
|
| 6 |
A1 |
1039 |
1000 |
0.06 |
|
|
|
| 7 |
A1 |
422 |
406 |
0.03 |
|
|
|
| 8 |
A2 |
778 |
748 |
0.00 |
|
|
|
| 9 |
A2 |
552 |
531 |
0.00 |
|
|
|
| 10 |
B1 |
1008 |
970 |
17.10 |
|
|
|
| 11 |
B1 |
800 |
770 |
62.20 |
|
|
|
| 12 |
B1 |
530 |
510 |
13.04 |
|
|
|
| 13 |
B2 |
3277 |
3153 |
3.36 |
|
|
|
| 14 |
B2 |
3164 |
3044 |
6.17 |
|
|
|
| 15 |
B2 |
1511 |
1453 |
0.13 |
|
|
|
| 16 |
B2 |
1400 |
1346 |
7.14 |
|
|
|
| 17 |
B2 |
1217 |
1171 |
0.07 |
|
|
|
| 18 |
B2 |
922 |
887 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14504.6 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 13952.0 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/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.444 |
| H2 |
0.000 |
0.000 |
1.540 |
| C3 |
0.000 |
1.228 |
-0.197 |
| C4 |
0.000 |
-1.228 |
-0.197 |
| H5 |
0.000 |
2.163 |
0.366 |
| H6 |
0.000 |
-2.163 |
0.366 |
| H7 |
0.000 |
1.292 |
-1.288 |
| H8 |
0.000 |
-1.292 |
-1.288 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0962 | 1.3851 | 1.3851 | 2.1644 | 2.1644 | 2.1608 | 2.1608 |
H2 | 1.0962 | | 2.1269 | 2.1269 | 2.4611 | 2.4611 | 3.1092 | 3.1092 | C3 | 1.3851 | 2.1269 | | 2.4564 | 1.0909 | 3.4375 | 1.0933 | 2.7468 | C4 | 1.3851 | 2.1269 | 2.4564 | | 3.4375 | 1.0909 | 2.7468 | 1.0933 | H5 | 2.1644 | 2.4611 | 1.0909 | 3.4375 | | 4.3259 | 1.8689 | 3.8308 | H6 | 2.1644 | 2.4611 | 3.4375 | 1.0909 | 4.3259 | | 3.8308 | 1.8689 | H7 | 2.1608 | 3.1092 | 1.0933 | 2.7468 | 1.8689 | 3.8308 | | 2.5849 | H8 | 2.1608 | 3.1092 | 2.7468 | 1.0933 | 3.8308 | 1.8689 | 2.5849 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.435 |
|
C1 |
C3 |
H7 |
120.903 |
| C1 |
C4 |
H6 |
121.435 |
|
C1 |
C4 |
H8 |
120.903 |
| H2 |
C1 |
C3 |
117.533 |
|
H2 |
C1 |
C4 |
117.533 |
| C3 |
C1 |
C4 |
124.934 |
|
H5 |
C3 |
H7 |
117.661 |
| H6 |
C4 |
H8 |
117.661 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.124 |
|
|
|
| 2 |
H |
0.014 |
|
|
|
| 3 |
C |
-0.034 |
|
|
|
| 4 |
C |
-0.034 |
|
|
|
| 5 |
H |
0.048 |
|
|
|
| 6 |
H |
0.048 |
|
|
|
| 7 |
H |
0.040 |
|
|
|
| 8 |
H |
0.040 |
|
|
|
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 |
-21.790 |
0.000 |
0.000 |
| y |
0.000 |
-17.702 |
0.000 |
| z |
0.000 |
0.000 |
-17.567 |
|
| Traceless |
| | x | y | z |
| x |
-4.156 |
0.000 |
0.000 |
| y |
0.000 |
1.977 |
0.000 |
| z |
0.000 |
0.000 |
2.178 |
|
| Polar |
| 3z2-r2 | 4.357 |
| x2-y2 | -4.088 |
| 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 |
2.234 |
0.000 |
0.000 |
| y |
0.000 |
7.715 |
0.000 |
| z |
0.000 |
0.000 |
4.828 |
<r2> (average value of r
2) Å
2
| <r2> |
50.280 |
| (<r2>)1/2 |
7.091 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -117.125314 |
| Energy at 298.15K | -117.129561 |
| HF Energy | -117.125314 |
| Nuclear repulsion energy | 64.749806 |
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/cc-pVDZ
| 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' |
3280 |
3155 |
11.85 |
|
|
|
| 2 |
A' |
3277 |
3153 |
3.72 |
|
|
|
| 3 |
A' |
3173 |
3052 |
0.37 |
|
|
|
| 4 |
A' |
3166 |
3046 |
15.06 |
|
|
|
| 5 |
A' |
3164 |
3044 |
6.22 |
|
|
|
| 6 |
A' |
1511 |
1453 |
0.12 |
|
|
|
| 7 |
A' |
1500 |
1443 |
2.37 |
|
|
|
| 8 |
A' |
1399 |
1346 |
7.16 |
|
|
|
| 9 |
A' |
1269 |
1220 |
1.45 |
|
|
|
| 10 |
A' |
1217 |
1171 |
0.07 |
|
|
|
| 11 |
A' |
1039 |
1000 |
0.06 |
|
|
|
| 12 |
A' |
923 |
887 |
0.13 |
|
|
|
| 13 |
A' |
422 |
406 |
0.03 |
|
|
|
| 14 |
A" |
1008 |
970 |
17.09 |
|
|
|
| 15 |
A" |
800 |
770 |
62.17 |
|
|
|
| 16 |
A" |
778 |
748 |
0.00 |
|
|
|
| 17 |
A" |
553 |
532 |
0.00 |
|
|
|
| 18 |
A" |
531 |
510 |
13.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14504.9 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 13952.2 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.444 |
0.000 |
| H2 |
0.000 |
1.540 |
0.000 |
| C3 |
-1.228 |
-0.197 |
0.000 |
| C4 |
1.228 |
-0.197 |
0.000 |
| H5 |
-2.163 |
0.366 |
0.000 |
| H6 |
2.163 |
0.366 |
0.000 |
| H7 |
-1.291 |
-1.288 |
0.000 |
| H8 |
1.291 |
-1.288 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0962 | 1.3850 | 1.3851 | 2.1644 | 2.1642 | 2.1603 | 2.1604 |
H2 | 1.0962 | | 2.1272 | 2.1268 | 2.4615 | 2.4608 | 3.1090 | 3.1089 | C3 | 1.3850 | 2.1272 | | 2.4561 | 1.0910 | 3.4372 | 1.0933 | 2.7456 | C4 | 1.3851 | 2.1268 | 2.4561 | | 3.4374 | 1.0908 | 2.7455 | 1.0933 | H5 | 2.1644 | 2.4615 | 1.0910 | 3.4374 | | 4.3258 | 1.8695 | 3.8298 | H6 | 2.1642 | 2.4608 | 3.4372 | 1.0908 | 4.3258 | | 3.8294 | 1.8694 | H7 | 2.1603 | 3.1090 | 1.0933 | 2.7455 | 1.8695 | 3.8294 | | 2.5824 | H8 | 2.1604 | 3.1089 | 2.7456 | 1.0933 | 3.8298 | 1.8694 | 2.5824 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.435 |
|
C1 |
C3 |
H7 |
120.852 |
| C1 |
C4 |
H6 |
121.426 |
|
C1 |
C4 |
H8 |
120.858 |
| H2 |
C1 |
C3 |
117.561 |
|
H2 |
C1 |
C4 |
117.528 |
| C3 |
C1 |
C4 |
124.911 |
|
H5 |
C3 |
H7 |
117.713 |
| H6 |
C4 |
H8 |
117.716 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.124 |
|
|
|
| 2 |
H |
0.014 |
|
|
|
| 3 |
C |
-0.034 |
|
|
|
| 4 |
C |
-0.034 |
|
|
|
| 5 |
H |
0.048 |
|
|
|
| 6 |
H |
0.048 |
|
|
|
| 7 |
H |
0.040 |
|
|
|
| 8 |
H |
0.040 |
|
|
|
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 |
-17.705 |
0.001 |
0.000 |
| y |
0.001 |
-17.567 |
0.000 |
| z |
0.000 |
0.000 |
-21.790 |
|
| Traceless |
| | x | y | z |
| x |
1.974 |
0.001 |
0.000 |
| y |
0.001 |
2.180 |
0.000 |
| z |
0.000 |
0.000 |
-4.155 |
|
| Polar |
| 3z2-r2 | -8.309 |
| x2-y2 | -0.138 |
| xy | 0.001 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.713 |
-0.000 |
0.000 |
| y |
-0.000 |
4.829 |
0.000 |
| z |
0.000 |
0.000 |
2.234 |
<r2> (average value of r
2) Å
2
| <r2> |
50.272 |
| (<r2>)1/2 |
7.090 |