Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -191.752518 |
| Energy at 298.15K | |
| HF Energy | -191.752518 |
| Nuclear repulsion energy | 103.351202 |
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' |
3247 |
3118 |
4.97 |
66.94 |
0.54 |
0.70 |
| 2 |
A' |
3195 |
3068 |
1.73 |
106.03 |
0.33 |
0.50 |
| 3 |
A' |
3149 |
3024 |
5.41 |
75.33 |
0.13 |
0.23 |
| 4 |
A' |
2890 |
2776 |
104.78 |
109.74 |
0.29 |
0.44 |
| 5 |
A' |
1821 |
1749 |
242.83 |
59.92 |
0.44 |
0.61 |
| 6 |
A' |
1698 |
1630 |
2.60 |
33.94 |
0.20 |
0.33 |
| 7 |
A' |
1451 |
1393 |
13.94 |
5.90 |
0.62 |
0.76 |
| 8 |
A' |
1388 |
1333 |
7.83 |
19.33 |
0.42 |
0.59 |
| 9 |
A' |
1293 |
1242 |
4.58 |
6.78 |
0.25 |
0.40 |
| 10 |
A' |
1173 |
1126 |
35.52 |
11.13 |
0.53 |
0.70 |
| 11 |
A' |
923 |
887 |
21.16 |
1.22 |
0.06 |
0.12 |
| 12 |
A' |
576 |
553 |
6.41 |
5.49 |
0.33 |
0.50 |
| 13 |
A' |
317 |
305 |
9.71 |
1.03 |
0.38 |
0.55 |
| 14 |
A" |
1044 |
1003 |
8.41 |
1.73 |
0.75 |
0.86 |
| 15 |
A" |
1032 |
992 |
8.31 |
3.41 |
0.75 |
0.86 |
| 16 |
A" |
1000 |
960 |
48.37 |
0.97 |
0.75 |
0.86 |
| 17 |
A" |
615 |
590 |
11.27 |
2.18 |
0.75 |
0.86 |
| 18 |
A" |
173 |
166 |
3.95 |
1.36 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13491.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 12957.3 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.152 |
-0.743 |
0.000 |
| C2 |
0.000 |
0.719 |
0.000 |
| C3 |
1.209 |
1.279 |
0.000 |
| O4 |
-1.211 |
-1.318 |
0.000 |
| H5 |
0.809 |
-1.305 |
0.000 |
| H6 |
-0.915 |
1.304 |
0.000 |
| H7 |
1.350 |
2.354 |
0.000 |
| H8 |
2.105 |
0.663 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4699 | 2.4371 | 1.2048 | 1.1135 | 2.1845 | 3.4418 | 2.6598 |
C2 | 1.4699 | | 1.3320 | 2.3693 | 2.1796 | 1.0861 | 2.1200 | 2.1061 | C3 | 2.4371 | 1.3320 | | 3.5490 | 2.6142 | 2.1240 | 1.0842 | 1.0874 | O4 | 1.2048 | 2.3693 | 3.5490 | | 2.0207 | 2.6378 | 4.4761 | 3.8631 | H5 | 1.1135 | 2.1796 | 2.6142 | 2.0207 | | 3.1271 | 3.6982 | 2.3567 | H6 | 2.1845 | 1.0861 | 2.1240 | 2.6378 | 3.1271 | | 2.4966 | 3.0876 | H7 | 3.4418 | 2.1200 | 1.0842 | 4.4761 | 3.6982 | 2.4966 | | 1.8512 | H8 | 2.6598 | 2.1061 | 1.0874 | 3.8631 | 2.3567 | 3.0876 | 1.8512 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.787 |
|
C1 |
C2 |
H6 |
116.639 |
| C2 |
C1 |
O4 |
124.404 |
|
C2 |
C1 |
H5 |
114.357 |
| C2 |
C3 |
H7 |
122.335 |
|
C2 |
C3 |
H8 |
120.699 |
| C3 |
C2 |
H6 |
122.574 |
|
O4 |
C1 |
H5 |
121.239 |
| H7 |
C3 |
H8 |
116.965 |
|
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 |
0.192 |
|
|
|
| 2 |
C |
-0.199 |
|
|
|
| 3 |
C |
-0.188 |
|
|
|
| 4 |
O |
-0.293 |
|
|
|
| 5 |
H |
0.074 |
|
|
|
| 6 |
H |
0.134 |
|
|
|
| 7 |
H |
0.145 |
|
|
|
| 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 |
| |
2.415 |
2.042 |
0.000 |
3.162 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.211 |
-2.562 |
0.000 |
| y |
-2.562 |
-23.789 |
0.000 |
| z |
0.000 |
0.000 |
-24.800 |
|
| Traceless |
| | x | y | z |
| x |
0.084 |
-2.562 |
0.000 |
| y |
-2.562 |
0.717 |
0.000 |
| z |
0.000 |
0.000 |
-0.800 |
|
| Polar |
| 3z2-r2 | -1.601 |
| x2-y2 | -0.422 |
| xy | -2.562 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.993 |
1.683 |
0.000 |
| y |
1.683 |
6.341 |
0.000 |
| z |
0.000 |
0.000 |
2.633 |
<r2> (average value of r
2) Å
2
| <r2> |
83.035 |
| (<r2>)1/2 |
9.112 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -191.749884 |
| Energy at 298.15K | |
| HF Energy | -191.749884 |
| Nuclear repulsion energy | 104.964709 |
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' |
3258 |
3129 |
1.87 |
57.24 |
0.62 |
0.77 |
| 2 |
A' |
3184 |
3058 |
10.34 |
124.86 |
0.27 |
0.42 |
| 3 |
A' |
3158 |
3033 |
5.09 |
57.53 |
0.15 |
0.26 |
| 4 |
A' |
2921 |
2805 |
149.77 |
176.65 |
0.31 |
0.47 |
| 5 |
A' |
1822 |
1750 |
121.32 |
14.27 |
0.61 |
0.76 |
| 6 |
A' |
1688 |
1621 |
68.40 |
47.86 |
0.20 |
0.33 |
| 7 |
A' |
1433 |
1377 |
32.86 |
8.16 |
0.70 |
0.83 |
| 8 |
A' |
1422 |
1365 |
15.99 |
7.52 |
0.26 |
0.41 |
| 9 |
A' |
1313 |
1261 |
2.76 |
16.09 |
0.38 |
0.55 |
| 10 |
A' |
1068 |
1026 |
5.35 |
4.37 |
0.68 |
0.81 |
| 11 |
A' |
944 |
906 |
62.66 |
4.12 |
0.18 |
0.31 |
| 12 |
A' |
687 |
659 |
11.11 |
0.77 |
0.71 |
0.83 |
| 13 |
A' |
289 |
277 |
7.29 |
3.54 |
0.46 |
0.63 |
| 14 |
A" |
1048 |
1006 |
3.47 |
8.22 |
0.75 |
0.86 |
| 15 |
A" |
1032 |
991 |
33.64 |
0.13 |
0.75 |
0.86 |
| 16 |
A" |
1015 |
975 |
18.87 |
0.47 |
0.75 |
0.86 |
| 17 |
A" |
565 |
543 |
11.28 |
3.77 |
0.75 |
0.86 |
| 18 |
A" |
181 |
174 |
7.49 |
0.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13513.4 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 12978.3 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.885 |
-0.290 |
0.000 |
| C2 |
0.000 |
0.897 |
0.000 |
| C3 |
1.325 |
0.766 |
0.000 |
| O4 |
-0.493 |
-1.430 |
0.000 |
| H5 |
-1.973 |
-0.068 |
0.000 |
| H6 |
-0.477 |
1.874 |
0.000 |
| H7 |
1.990 |
1.622 |
0.000 |
| H8 |
1.765 |
-0.227 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4808 | 2.4494 | 1.2056 | 1.1105 | 2.2018 | 3.4527 | 2.6514 |
C2 | 1.4808 | | 1.3314 | 2.3787 | 2.1967 | 1.0866 | 2.1177 | 2.0927 | C3 | 2.4494 | 1.3314 | | 2.8506 | 3.4020 | 2.1150 | 1.0840 | 1.0858 | O4 | 1.2056 | 2.3787 | 2.8506 | | 2.0116 | 3.3036 | 3.9342 | 2.5589 | H5 | 1.1105 | 2.1967 | 3.4020 | 2.0116 | | 2.4514 | 4.3083 | 3.7421 | H6 | 2.2018 | 1.0866 | 2.1150 | 3.3036 | 2.4514 | | 2.4793 | 3.0722 | H7 | 3.4527 | 2.1177 | 1.0840 | 3.9342 | 4.3083 | 2.4793 | | 1.8623 | H8 | 2.6514 | 2.0927 | 1.0858 | 2.5589 | 3.7421 | 3.0722 | 1.8623 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.054 |
|
C1 |
C2 |
H6 |
117.263 |
| C2 |
C1 |
O4 |
124.295 |
|
C2 |
C1 |
H5 |
115.183 |
| C2 |
C3 |
H7 |
122.169 |
|
C2 |
C3 |
H8 |
119.594 |
| C3 |
C2 |
H6 |
121.683 |
|
O4 |
C1 |
H5 |
120.522 |
| H7 |
C3 |
H8 |
118.238 |
|
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 |
0.193 |
|
|
|
| 2 |
C |
-0.248 |
|
|
|
| 3 |
C |
-0.146 |
|
|
|
| 4 |
O |
-0.292 |
|
|
|
| 5 |
H |
0.083 |
|
|
|
| 6 |
H |
0.122 |
|
|
|
| 7 |
H |
0.138 |
|
|
|
| 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 |
| |
0.234 |
2.629 |
0.000 |
2.640 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.072 |
-0.611 |
0.000 |
| y |
-0.611 |
-25.922 |
0.000 |
| z |
0.000 |
0.000 |
-24.772 |
|
| Traceless |
| | x | y | z |
| x |
5.275 |
-0.611 |
0.000 |
| y |
-0.611 |
-3.500 |
0.000 |
| z |
0.000 |
0.000 |
-1.775 |
|
| Polar |
| 3z2-r2 | -3.550 |
| x2-y2 | 5.850 |
| xy | -0.611 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.180 |
0.447 |
0.000 |
| y |
0.447 |
5.687 |
0.000 |
| z |
0.000 |
0.000 |
2.619 |
<r2> (average value of r
2) Å
2
| <r2> |
74.515 |
| (<r2>)1/2 |
8.632 |