Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -190.633701 |
| Energy at 298.15K | |
| HF Energy | -190.633701 |
| Nuclear repulsion energy | 88.746292 |
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 wB97X-D/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 |
3096 |
2961 |
29.91 |
192.62 |
0.13 |
0.23 |
| 2 |
A1 |
2370 |
2267 |
1041.43 |
38.94 |
0.36 |
0.53 |
| 3 |
A1 |
1832 |
1752 |
34.65 |
0.19 |
0.12 |
0.22 |
| 4 |
A1 |
1483 |
1418 |
1.66 |
14.61 |
0.58 |
0.73 |
| 5 |
A1 |
941 |
900 |
5.19 |
42.38 |
0.27 |
0.42 |
| 6 |
B1 |
1037 |
992 |
23.68 |
0.95 |
0.75 |
0.86 |
| 7 |
B1 |
669 |
640 |
31.76 |
1.67 |
0.75 |
0.86 |
| 8 |
B1 |
220 |
211 |
0.93 |
4.06 |
0.75 |
0.86 |
| 9 |
B2 |
3172 |
3034 |
9.09 |
125.40 |
0.75 |
0.86 |
| 10 |
B2 |
1071 |
1025 |
2.14 |
0.08 |
0.75 |
0.86 |
| 11 |
B2 |
487 |
466 |
18.41 |
2.55 |
0.75 |
0.86 |
| 12 |
B2 |
106i |
101i |
20.26 |
0.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8136.2 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 7782.2 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 wB97X-D/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.866 |
| C2 |
0.000 |
0.000 |
-0.554 |
| C3 |
0.000 |
0.000 |
0.719 |
| O4 |
0.000 |
0.000 |
1.887 |
| H5 |
0.000 |
0.925 |
-2.442 |
| H6 |
0.000 |
-0.925 |
-2.442 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3120 | 2.5853 | 3.7533 | 1.0895 | 1.0895 |
C2 | 1.3120 | | 1.2733 | 2.4413 | 2.1020 | 2.1020 | C3 | 2.5853 | 1.2733 | | 1.1680 | 3.2935 | 3.2935 | O4 | 3.7533 | 2.4413 | 1.1680 | | 4.4266 | 4.4266 | H5 | 1.0895 | 2.1020 | 3.2935 | 4.4266 | | 1.8502 | H6 | 1.0895 | 2.1020 | 3.2935 | 4.4266 | 1.8502 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
121.889 |
| C2 |
C1 |
H6 |
121.889 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
116.222 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.140 |
|
|
|
| 2 |
C |
-0.158 |
|
|
|
| 3 |
C |
0.221 |
|
|
|
| 4 |
O |
-0.232 |
|
|
|
| 5 |
H |
0.155 |
|
|
|
| 6 |
H |
0.155 |
|
|
|
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 |
-2.718 |
2.718 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.545 |
0.000 |
0.000 |
| y |
0.000 |
-22.309 |
0.000 |
| z |
0.000 |
0.000 |
-21.442 |
|
| Traceless |
| | x | y | z |
| x |
-0.670 |
0.000 |
0.000 |
| y |
0.000 |
-0.315 |
0.000 |
| z |
0.000 |
0.000 |
0.985 |
|
| Polar |
| 3z2-r2 | 1.970 |
| x2-y2 | -0.237 |
| 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 |
2.257 |
0.000 |
0.000 |
| y |
0.000 |
2.907 |
0.000 |
| z |
0.000 |
0.000 |
10.349 |
<r2> (average value of r
2) Å
2
| <r2> |
81.768 |
| (<r2>)1/2 |
9.043 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -190.634119 |
| Energy at 298.15K | |
| HF Energy | -190.634119 |
| Nuclear repulsion energy | 88.911919 |
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 wB97X-D/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' |
3181 |
3042 |
9.07 |
117.70 |
0.70 |
0.83 |
| 2 |
A' |
3099 |
2964 |
29.06 |
160.57 |
0.13 |
0.23 |
| 3 |
A' |
2305 |
2205 |
1059.49 |
42.06 |
0.39 |
0.56 |
| 4 |
A' |
1813 |
1734 |
14.25 |
2.55 |
0.36 |
0.53 |
| 5 |
A' |
1487 |
1422 |
0.91 |
15.26 |
0.59 |
0.75 |
| 6 |
A' |
1074 |
1028 |
13.86 |
4.20 |
0.10 |
0.18 |
| 7 |
A' |
957 |
915 |
3.24 |
36.60 |
0.22 |
0.36 |
| 8 |
A' |
511 |
489 |
17.89 |
5.03 |
0.58 |
0.73 |
| 9 |
A' |
125 |
119 |
24.04 |
5.75 |
0.72 |
0.84 |
| 10 |
A" |
1040 |
995 |
24.13 |
1.16 |
0.75 |
0.86 |
| 11 |
A" |
707 |
676 |
24.88 |
2.47 |
0.75 |
0.86 |
| 12 |
A" |
262 |
250 |
0.64 |
5.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8279.8 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 7919.6 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 wB97X-D/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.858 |
-1.618 |
0.000 |
| C2 |
0.000 |
-0.619 |
0.000 |
| C3 |
-0.298 |
0.635 |
0.000 |
| O4 |
-0.728 |
1.716 |
0.000 |
| H5 |
1.937 |
-1.463 |
0.000 |
| H6 |
0.524 |
-2.654 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3175 | 2.5329 | 3.6927 | 1.0899 | 1.0881 |
C2 | 1.3175 | | 1.2888 | 2.4459 | 2.1128 | 2.1012 | C3 | 2.5329 | 1.2888 | | 1.1635 | 3.0654 | 3.3899 | O4 | 3.6927 | 2.4459 | 1.1635 | | 4.1480 | 4.5457 | H5 | 1.0899 | 2.1128 | 3.0654 | 4.1480 | | 1.8485 | H6 | 1.0881 | 2.1012 | 3.3899 | 4.5457 | 1.8485 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
152.730 |
|
C2 |
C1 |
H5 |
122.430 |
| C2 |
C1 |
H6 |
121.429 |
|
C2 |
C3 |
O4 |
171.727 |
| H5 |
C1 |
H6 |
116.141 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.172 |
|
|
|
| 2 |
C |
-0.215 |
|
|
|
| 3 |
C |
0.312 |
|
|
|
| 4 |
O |
-0.226 |
|
|
|
| 5 |
H |
0.149 |
|
|
|
| 6 |
H |
0.152 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.684 |
-1.876 |
0.000 |
2.521 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.830 |
-0.915 |
0.000 |
| y |
-0.915 |
-22.279 |
0.000 |
| z |
0.000 |
0.000 |
-22.619 |
|
| Traceless |
| | x | y | z |
| x |
0.619 |
-0.915 |
0.000 |
| y |
-0.915 |
-0.054 |
0.000 |
| z |
0.000 |
0.000 |
-0.565 |
|
| Polar |
| 3z2-r2 | -1.130 |
| x2-y2 | 0.449 |
| xy | -0.915 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.478 |
-2.570 |
0.000 |
| y |
-2.570 |
8.878 |
0.000 |
| z |
0.000 |
0.000 |
2.297 |
<r2> (average value of r
2) Å
2
| <r2> |
80.290 |
| (<r2>)1/2 |
8.960 |