Jump to
S1C2
Energy calculated at B1B95/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -191.853967 |
| Energy at 298.15K | |
| HF Energy | -191.853967 |
| Nuclear repulsion energy | 103.175591 |
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 B1B95/daug-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' |
3270 |
3270 |
4.15 |
65.45 |
0.54 |
0.70 |
| 2 |
A' |
3218 |
3218 |
1.12 |
104.77 |
0.27 |
0.43 |
| 3 |
A' |
3165 |
3165 |
4.55 |
88.43 |
0.08 |
0.15 |
| 4 |
A' |
2924 |
2924 |
85.65 |
111.70 |
0.27 |
0.42 |
| 5 |
A' |
1806 |
1806 |
276.90 |
89.51 |
0.37 |
0.54 |
| 6 |
A' |
1700 |
1700 |
2.10 |
50.92 |
0.12 |
0.21 |
| 7 |
A' |
1445 |
1445 |
13.07 |
5.51 |
0.51 |
0.67 |
| 8 |
A' |
1373 |
1373 |
6.28 |
19.71 |
0.30 |
0.46 |
| 9 |
A' |
1291 |
1291 |
4.01 |
9.45 |
0.14 |
0.25 |
| 10 |
A' |
1175 |
1175 |
37.67 |
11.35 |
0.64 |
0.78 |
| 11 |
A' |
920 |
920 |
16.53 |
1.76 |
0.00 |
0.01 |
| 12 |
A' |
572 |
572 |
5.10 |
6.13 |
0.17 |
0.28 |
| 13 |
A' |
316 |
316 |
10.45 |
1.17 |
0.31 |
0.48 |
| 14 |
A" |
1048 |
1048 |
4.20 |
1.20 |
0.75 |
0.86 |
| 15 |
A" |
1039 |
1039 |
8.37 |
1.77 |
0.75 |
0.86 |
| 16 |
A" |
1018 |
1018 |
44.93 |
1.46 |
0.75 |
0.86 |
| 17 |
A" |
622 |
622 |
10.11 |
0.66 |
0.75 |
0.86 |
| 18 |
A" |
173 |
173 |
4.42 |
0.51 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13536.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13536.2 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 B1B95/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.153 |
-0.741 |
0.000 |
| C2 |
0.000 |
0.721 |
0.000 |
| C3 |
1.216 |
1.273 |
0.000 |
| O4 |
-1.218 |
-1.315 |
0.000 |
| H5 |
0.804 |
-1.311 |
0.000 |
| H6 |
-0.913 |
1.314 |
0.000 |
| H7 |
1.364 |
2.350 |
0.000 |
| H8 |
2.109 |
0.649 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4692 | 2.4351 | 1.2097 | 1.1137 | 2.1903 | 3.4426 | 2.6546 |
C2 | 1.4692 | | 1.3358 | 2.3718 | 2.1847 | 1.0885 | 2.1247 | 2.1102 | C3 | 2.4351 | 1.3358 | | 3.5526 | 2.6168 | 2.1292 | 1.0868 | 1.0894 | O4 | 1.2097 | 2.3718 | 3.5526 | | 2.0214 | 2.6460 | 4.4825 | 3.8630 | H5 | 1.1137 | 2.1847 | 2.6168 | 2.0214 | | 3.1360 | 3.7033 | 2.3547 | H6 | 2.1903 | 1.0885 | 2.1292 | 2.6460 | 3.1360 | | 2.5012 | 3.0939 | H7 | 3.4426 | 2.1247 | 1.0868 | 4.4825 | 3.7033 | 2.5012 | | 1.8570 | H8 | 2.6546 | 2.1102 | 1.0894 | 3.8630 | 2.3547 | 3.0939 | 1.8570 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.410 |
|
C1 |
C2 |
H6 |
117.041 |
| C2 |
C1 |
O4 |
124.304 |
|
C2 |
C1 |
H5 |
114.824 |
| C2 |
C3 |
H7 |
122.244 |
|
C2 |
C3 |
H8 |
120.604 |
| C3 |
C2 |
H6 |
122.549 |
|
O4 |
C1 |
H5 |
120.873 |
| H7 |
C3 |
H8 |
117.153 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
2.327 |
|
|
|
| 2 |
C |
1.690 |
|
|
|
| 3 |
C |
0.316 |
|
|
|
| 4 |
O |
-0.505 |
|
|
|
| 5 |
H |
-0.996 |
|
|
|
| 6 |
H |
-0.939 |
|
|
|
| 7 |
H |
-1.098 |
|
|
|
| 8 |
H |
-0.795 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.577 |
2.180 |
0.000 |
3.376 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.734 |
-2.720 |
0.000 |
| y |
-2.720 |
-24.044 |
0.000 |
| z |
0.000 |
0.000 |
-25.001 |
|
| Traceless |
| | x | y | z |
| x |
-0.211 |
-2.720 |
0.000 |
| y |
-2.720 |
0.823 |
0.000 |
| z |
0.000 |
0.000 |
-0.612 |
|
| Polar |
| 3z2-r2 | -1.225 |
| x2-y2 | -0.690 |
| xy | -2.720 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.764 |
1.718 |
0.000 |
| y |
1.718 |
7.315 |
0.000 |
| z |
0.000 |
0.000 |
4.196 |
<r2> (average value of r
2) Å
2
| <r2> |
83.371 |
| (<r2>)1/2 |
9.131 |
Jump to
S1C1
Energy calculated at B1B95/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -191.850397 |
| Energy at 298.15K | |
| HF Energy | -191.850397 |
| Nuclear repulsion energy | 104.730451 |
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 B1B95/daug-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' |
3282 |
3282 |
1.37 |
55.19 |
0.61 |
0.76 |
| 2 |
A' |
3206 |
3206 |
9.89 |
125.52 |
0.22 |
0.36 |
| 3 |
A' |
3174 |
3174 |
4.76 |
72.49 |
0.10 |
0.17 |
| 4 |
A' |
2949 |
2949 |
130.08 |
181.98 |
0.29 |
0.44 |
| 5 |
A' |
1806 |
1806 |
129.39 |
20.62 |
0.60 |
0.75 |
| 6 |
A' |
1693 |
1693 |
70.49 |
73.24 |
0.13 |
0.23 |
| 7 |
A' |
1425 |
1425 |
35.51 |
5.44 |
0.66 |
0.80 |
| 8 |
A' |
1410 |
1410 |
8.90 |
9.07 |
0.12 |
0.21 |
| 9 |
A' |
1305 |
1305 |
2.65 |
21.36 |
0.27 |
0.42 |
| 10 |
A' |
1059 |
1059 |
3.34 |
2.78 |
0.73 |
0.85 |
| 11 |
A' |
947 |
947 |
60.99 |
6.90 |
0.07 |
0.13 |
| 12 |
A' |
678 |
678 |
13.34 |
0.62 |
0.74 |
0.85 |
| 13 |
A' |
279 |
279 |
7.21 |
3.46 |
0.30 |
0.46 |
| 14 |
A" |
1051 |
1051 |
0.38 |
4.77 |
0.75 |
0.86 |
| 15 |
A" |
1033 |
1033 |
45.92 |
0.42 |
0.75 |
0.86 |
| 16 |
A" |
1025 |
1025 |
3.29 |
0.11 |
0.75 |
0.86 |
| 17 |
A" |
563 |
563 |
10.10 |
0.89 |
0.75 |
0.86 |
| 18 |
A" |
154 |
154 |
6.39 |
0.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13519.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13519.2 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 B1B95/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.888 |
-0.288 |
0.000 |
| C2 |
0.000 |
0.896 |
0.000 |
| C3 |
1.329 |
0.768 |
0.000 |
| O4 |
-0.495 |
-1.433 |
0.000 |
| H5 |
-1.978 |
-0.073 |
0.000 |
| H6 |
-0.478 |
1.874 |
0.000 |
| H7 |
1.987 |
1.633 |
0.000 |
| H8 |
1.778 |
-0.223 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4798 | 2.4556 | 1.2104 | 1.1111 | 2.2011 | 3.4578 | 2.6666 |
C2 | 1.4798 | | 1.3351 | 2.3809 | 2.2019 | 1.0891 | 2.1197 | 2.1009 | C3 | 2.4556 | 1.3351 | | 2.8588 | 3.4119 | 2.1186 | 1.0867 | 1.0884 | O4 | 1.2104 | 2.3809 | 2.8588 | | 2.0124 | 3.3076 | 3.9449 | 2.5751 | H5 | 1.1111 | 2.2019 | 3.4119 | 2.0124 | | 2.4576 | 4.3163 | 3.7588 | H6 | 2.2011 | 1.0891 | 2.1186 | 3.3076 | 2.4576 | | 2.4771 | 3.0804 | H7 | 3.4578 | 2.1197 | 1.0867 | 3.9449 | 4.3163 | 2.4771 | | 1.8676 | H8 | 2.6666 | 2.1009 | 1.0884 | 2.5751 | 3.7588 | 3.0804 | 1.8676 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.381 |
|
C1 |
C2 |
H6 |
117.114 |
| C2 |
C1 |
O4 |
124.206 |
|
C2 |
C1 |
H5 |
115.666 |
| C2 |
C3 |
H7 |
121.816 |
|
C2 |
C3 |
H8 |
119.850 |
| C3 |
C2 |
H6 |
121.505 |
|
O4 |
C1 |
H5 |
120.128 |
| H7 |
C3 |
H8 |
118.335 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.259 |
|
|
|
| 2 |
C |
2.035 |
|
|
|
| 3 |
C |
0.503 |
|
|
|
| 4 |
O |
-0.589 |
|
|
|
| 5 |
H |
-0.645 |
|
|
|
| 6 |
H |
-0.983 |
|
|
|
| 7 |
H |
-0.807 |
|
|
|
| 8 |
H |
-0.773 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.235 |
2.755 |
0.000 |
2.765 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.275 |
-0.679 |
0.000 |
| y |
-0.679 |
-26.468 |
0.000 |
| z |
0.000 |
0.000 |
-24.965 |
|
| Traceless |
| | x | y | z |
| x |
5.441 |
-0.679 |
0.000 |
| y |
-0.679 |
-3.848 |
0.000 |
| z |
0.000 |
0.000 |
-1.594 |
|
| Polar |
| 3z2-r2 | -3.187 |
| x2-y2 | 6.192 |
| xy | -0.679 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.874 |
0.619 |
0.000 |
| y |
0.619 |
6.672 |
0.000 |
| z |
0.000 |
0.000 |
4.174 |
<r2> (average value of r
2) Å
2
| <r2> |
74.985 |
| (<r2>)1/2 |
8.659 |