Jump to
S1C2
Energy calculated at HSEh1PBE/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -191.775897 |
| Energy at 298.15K | |
| HF Energy | -191.775897 |
| Nuclear repulsion energy | 103.508098 |
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/daug-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 |
A' |
3244 |
3244 |
3.06 |
64.84 |
0.51 |
0.67 |
| 2 |
A' |
3192 |
3192 |
0.97 |
101.21 |
0.28 |
0.44 |
| 3 |
A' |
3147 |
3147 |
4.25 |
84.75 |
0.08 |
0.14 |
| 4 |
A' |
2897 |
2897 |
84.82 |
111.08 |
0.26 |
0.42 |
| 5 |
A' |
1803 |
1803 |
272.63 |
84.80 |
0.38 |
0.55 |
| 6 |
A' |
1692 |
1692 |
2.51 |
51.29 |
0.12 |
0.22 |
| 7 |
A' |
1452 |
1452 |
13.83 |
6.07 |
0.47 |
0.64 |
| 8 |
A' |
1386 |
1386 |
6.70 |
20.09 |
0.29 |
0.45 |
| 9 |
A' |
1298 |
1298 |
3.67 |
9.74 |
0.14 |
0.25 |
| 10 |
A' |
1178 |
1178 |
38.43 |
12.17 |
0.61 |
0.76 |
| 11 |
A' |
925 |
925 |
18.99 |
1.61 |
0.00 |
0.00 |
| 12 |
A' |
576 |
576 |
4.91 |
6.12 |
0.16 |
0.27 |
| 13 |
A' |
320 |
320 |
10.14 |
1.25 |
0.31 |
0.48 |
| 14 |
A" |
1041 |
1041 |
9.72 |
0.41 |
0.75 |
0.86 |
| 15 |
A" |
1034 |
1034 |
3.88 |
2.03 |
0.75 |
0.86 |
| 16 |
A" |
1005 |
1005 |
44.12 |
2.26 |
0.75 |
0.86 |
| 17 |
A" |
617 |
617 |
10.66 |
0.63 |
0.75 |
0.86 |
| 18 |
A" |
170 |
170 |
4.32 |
0.52 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13487.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13487.6 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 HSEh1PBE/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.152 |
-0.739 |
0.000 |
| C2 |
0.000 |
0.719 |
0.000 |
| C3 |
1.209 |
1.272 |
0.000 |
| O4 |
-1.211 |
-1.315 |
0.000 |
| H5 |
0.804 |
-1.304 |
0.000 |
| H6 |
-0.911 |
1.308 |
0.000 |
| H7 |
1.354 |
2.345 |
0.000 |
| H8 |
2.100 |
0.652 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4662 | 2.4287 | 1.2054 | 1.1106 | 2.1826 | 3.4322 | 2.6473 |
C2 | 1.4662 | | 1.3296 | 2.3673 | 2.1770 | 1.0842 | 2.1159 | 2.1010 | C3 | 2.4287 | 1.3296 | | 3.5427 | 2.6076 | 2.1200 | 1.0823 | 1.0853 | O4 | 1.2054 | 2.3673 | 3.5427 | | 2.0154 | 2.6395 | 4.4693 | 3.8514 | H5 | 1.1106 | 2.1770 | 2.6076 | 2.0154 | | 3.1240 | 3.6897 | 2.3463 | H6 | 2.1826 | 1.0842 | 2.1200 | 2.6395 | 3.1240 | | 2.4913 | 3.0810 | H7 | 3.4322 | 2.1159 | 1.0823 | 4.4693 | 3.6897 | 2.4913 | | 1.8493 | H8 | 2.6473 | 2.1010 | 1.0853 | 3.8514 | 2.3463 | 3.0810 | 1.8493 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.535 |
|
C1 |
C2 |
H6 |
116.908 |
| C2 |
C1 |
O4 |
124.486 |
|
C2 |
C1 |
H5 |
114.603 |
| C2 |
C3 |
H7 |
122.297 |
|
C2 |
C3 |
H8 |
120.589 |
| C3 |
C2 |
H6 |
122.557 |
|
O4 |
C1 |
H5 |
120.911 |
| H7 |
C3 |
H8 |
117.115 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.309 |
|
|
|
| 2 |
C |
-0.151 |
|
|
|
| 3 |
C |
-1.225 |
|
|
|
| 4 |
O |
-0.960 |
|
|
|
| 5 |
H |
0.620 |
|
|
|
| 6 |
H |
0.461 |
|
|
|
| 7 |
H |
0.441 |
|
|
|
| 8 |
H |
0.504 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.568 |
2.191 |
0.000 |
3.375 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.678 |
-2.693 |
0.000 |
| y |
-2.693 |
-24.017 |
0.000 |
| z |
0.000 |
0.000 |
-25.010 |
|
| Traceless |
| | x | y | z |
| x |
-0.165 |
-2.693 |
0.000 |
| y |
-2.693 |
0.828 |
0.000 |
| z |
0.000 |
0.000 |
-0.662 |
|
| Polar |
| 3z2-r2 | -1.325 |
| x2-y2 | -0.662 |
| xy | -2.693 |
| 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 |
1.708 |
0.000 |
| y |
1.708 |
7.276 |
0.000 |
| z |
0.000 |
0.000 |
4.196 |
<r2> (average value of r
2) Å
2
| <r2> |
82.966 |
| (<r2>)1/2 |
9.109 |
Jump to
S1C1
Energy calculated at HSEh1PBE/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -191.772080 |
| Energy at 298.15K | |
| HF Energy | -191.772080 |
| Nuclear repulsion energy | 104.996277 |
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/daug-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 |
A' |
3254 |
3254 |
0.94 |
54.47 |
0.60 |
0.75 |
| 2 |
A' |
3180 |
3180 |
8.93 |
129.29 |
0.21 |
0.35 |
| 3 |
A' |
3156 |
3156 |
4.50 |
64.29 |
0.10 |
0.18 |
| 4 |
A' |
2920 |
2920 |
130.23 |
178.25 |
0.28 |
0.44 |
| 5 |
A' |
1807 |
1807 |
129.13 |
21.14 |
0.60 |
0.75 |
| 6 |
A' |
1684 |
1684 |
69.50 |
71.34 |
0.13 |
0.23 |
| 7 |
A' |
1434 |
1434 |
44.14 |
5.80 |
0.73 |
0.84 |
| 8 |
A' |
1423 |
1423 |
3.65 |
9.87 |
0.10 |
0.19 |
| 9 |
A' |
1313 |
1313 |
2.54 |
21.43 |
0.26 |
0.41 |
| 10 |
A' |
1069 |
1069 |
4.40 |
3.29 |
0.68 |
0.81 |
| 11 |
A' |
942 |
942 |
62.24 |
6.45 |
0.07 |
0.12 |
| 12 |
A' |
683 |
683 |
12.42 |
0.56 |
0.75 |
0.85 |
| 13 |
A' |
283 |
283 |
6.99 |
3.46 |
0.30 |
0.46 |
| 14 |
A" |
1045 |
1045 |
1.44 |
4.31 |
0.75 |
0.86 |
| 15 |
A" |
1030 |
1030 |
38.39 |
0.26 |
0.75 |
0.86 |
| 16 |
A" |
1021 |
1021 |
10.07 |
0.94 |
0.75 |
0.86 |
| 17 |
A" |
558 |
558 |
10.44 |
0.81 |
0.75 |
0.86 |
| 18 |
A" |
144 |
144 |
6.43 |
0.24 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13473.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13473.1 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 HSEh1PBE/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.882 |
-0.293 |
0.000 |
| C2 |
0.000 |
0.892 |
0.000 |
| C3 |
1.324 |
0.777 |
0.000 |
| O4 |
-0.494 |
-1.435 |
0.000 |
| H5 |
-1.969 |
-0.074 |
0.000 |
| H6 |
-0.483 |
1.863 |
0.000 |
| H7 |
1.972 |
1.643 |
0.000 |
| H8 |
1.783 |
-0.205 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4778 | 2.4520 | 1.2056 | 1.1083 | 2.1933 | 3.4495 | 2.6664 |
C2 | 1.4778 | | 1.3288 | 2.3786 | 2.1927 | 1.0847 | 2.1104 | 2.0933 | C3 | 2.4520 | 1.3288 | | 2.8626 | 3.4004 | 2.1085 | 1.0822 | 1.0839 | O4 | 1.2056 | 2.3786 | 2.8626 | | 2.0069 | 3.2979 | 3.9440 | 2.5873 | H5 | 1.1083 | 2.1927 | 3.4004 | 2.0069 | | 2.4408 | 4.2986 | 3.7535 | H6 | 2.1933 | 1.0847 | 2.1085 | 3.2979 | 2.4408 | | 2.4654 | 3.0680 | H7 | 3.4495 | 2.1104 | 1.0822 | 3.9440 | 4.2986 | 2.4654 | | 1.8581 | H8 | 2.6664 | 2.0933 | 1.0839 | 2.5873 | 3.7535 | 3.0680 | 1.8581 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.682 |
|
C1 |
C2 |
H6 |
116.886 |
| C2 |
C1 |
O4 |
124.542 |
|
C2 |
C1 |
H5 |
115.218 |
| C2 |
C3 |
H7 |
121.839 |
|
C2 |
C3 |
H8 |
120.021 |
| C3 |
C2 |
H6 |
121.432 |
|
O4 |
C1 |
H5 |
120.241 |
| H7 |
C3 |
H8 |
118.139 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.382 |
|
|
|
| 2 |
C |
-0.204 |
|
|
|
| 3 |
C |
-1.084 |
|
|
|
| 4 |
O |
-1.139 |
|
|
|
| 5 |
H |
0.859 |
|
|
|
| 6 |
H |
0.443 |
|
|
|
| 7 |
H |
0.464 |
|
|
|
| 8 |
H |
0.278 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.252 |
2.755 |
0.000 |
2.767 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.259 |
-0.646 |
0.000 |
| y |
-0.646 |
-26.440 |
0.000 |
| z |
0.000 |
0.000 |
-24.980 |
|
| Traceless |
| | x | y | z |
| x |
5.451 |
-0.646 |
0.000 |
| y |
-0.646 |
-3.821 |
0.000 |
| z |
0.000 |
0.000 |
-1.630 |
|
| Polar |
| 3z2-r2 | -3.260 |
| x2-y2 | 6.181 |
| xy | -0.646 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.835 |
0.621 |
0.000 |
| y |
0.621 |
6.636 |
0.000 |
| z |
0.000 |
0.000 |
4.177 |
<r2> (average value of r
2) Å
2
| <r2> |
74.834 |
| (<r2>)1/2 |
8.651 |