Jump to
S1C2
Energy calculated at wB97X-D/LANL2DZ
| hartrees |
Energy at 0K | -190.547123 |
Energy at 298.15K | |
HF Energy | -190.547123 |
Nuclear repulsion energy | 87.366083 |
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/LANL2DZ
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 |
3139 |
3139 |
29.17 |
183.36 |
0.11 |
0.20 |
2 |
A1 |
2334 |
2334 |
890.31 |
61.01 |
0.32 |
0.48 |
3 |
A1 |
1767 |
1767 |
75.62 |
0.40 |
0.10 |
0.19 |
4 |
A1 |
1500 |
1500 |
1.17 |
16.97 |
0.64 |
0.78 |
5 |
A1 |
917 |
917 |
9.57 |
49.51 |
0.28 |
0.44 |
6 |
B1 |
1065 |
1065 |
40.36 |
3.08 |
0.75 |
0.86 |
7 |
B1 |
655 |
655 |
33.39 |
3.74 |
0.75 |
0.86 |
8 |
B1 |
233 |
233 |
1.27 |
3.95 |
0.75 |
0.86 |
9 |
B2 |
3238 |
3238 |
14.61 |
108.03 |
0.75 |
0.86 |
10 |
B2 |
1082 |
1082 |
0.73 |
0.10 |
0.75 |
0.86 |
11 |
B2 |
452 |
452 |
19.83 |
2.58 |
0.75 |
0.86 |
12 |
B2 |
118 |
118 |
24.72 |
0.21 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8249.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8249.2 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/LANL2DZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
-1.894 |
C2 |
0.000 |
0.000 |
-0.565 |
C3 |
0.000 |
0.000 |
0.718 |
O4 |
0.000 |
0.000 |
1.922 |
H5 |
0.000 |
0.927 |
-2.467 |
H6 |
0.000 |
-0.927 |
-2.467 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
C1 | | 1.3287 | 2.6118 | 3.8154 | 1.0902 | 1.0902 |
C2 | 1.3287 | | 1.2831 | 2.4867 | 2.1162 | 2.1162 | C3 | 2.6118 | 1.2831 | | 1.2036 | 3.3175 | 3.3175 | O4 | 3.8154 | 2.4867 | 1.2036 | | 4.4858 | 4.4858 | H5 | 1.0902 | 2.1162 | 3.3175 | 4.4858 | | 1.8544 | H6 | 1.0902 | 2.1162 | 3.3175 | 4.4858 | 1.8544 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
121.737 |
C2 |
C1 |
H6 |
121.737 |
|
C2 |
C3 |
O4 |
180.000 |
H5 |
C1 |
H6 |
116.526 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.411 |
|
|
|
2 |
C |
-0.130 |
|
|
|
3 |
C |
0.256 |
|
|
|
4 |
O |
-0.187 |
|
|
|
5 |
H |
0.236 |
|
|
|
6 |
H |
0.236 |
|
|
|
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 |
-3.388 |
3.388 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.791 |
0.000 |
0.000 |
y |
0.000 |
-22.331 |
0.000 |
z |
0.000 |
0.000 |
-22.194 |
|
Traceless |
| x | y | z |
x |
-0.528 |
0.000 |
0.000 |
y |
0.000 |
0.161 |
0.000 |
z |
0.000 |
0.000 |
0.367 |
|
Polar |
3z2-r2 | 0.734 |
x2-y2 | -0.460 |
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 |
1.849 |
0.000 |
0.000 |
y |
0.000 |
2.514 |
0.000 |
z |
0.000 |
0.000 |
10.735 |
<r2> (average value of r
2) Å
2
<r2> |
83.979 |
(<r2>)1/2 |
9.164 |
Jump to
S1C1
Energy calculated at wB97X-D/LANL2DZ
| hartrees |
Energy at 0K | -190.547123 |
Energy at 298.15K | |
HF Energy | -190.547123 |
Nuclear repulsion energy | 87.368248 |
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/LANL2DZ
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' |
3238 |
3238 |
14.58 |
107.97 |
0.75 |
0.86 |
2 |
A' |
3139 |
3139 |
29.14 |
183.29 |
0.11 |
0.20 |
3 |
A' |
2334 |
2334 |
890.38 |
61.05 |
0.32 |
0.48 |
4 |
A' |
1767 |
1767 |
75.55 |
0.40 |
0.10 |
0.19 |
5 |
A' |
1500 |
1500 |
1.17 |
16.94 |
0.64 |
0.78 |
6 |
A' |
1082 |
1082 |
0.73 |
0.10 |
0.75 |
0.86 |
7 |
A' |
917 |
917 |
9.59 |
49.53 |
0.28 |
0.44 |
8 |
A' |
452 |
452 |
19.82 |
2.58 |
0.75 |
0.86 |
9 |
A' |
118 |
118 |
24.73 |
0.22 |
0.75 |
0.86 |
10 |
A" |
1065 |
1065 |
40.37 |
3.08 |
0.75 |
0.86 |
11 |
A" |
655 |
655 |
33.40 |
3.74 |
0.75 |
0.86 |
12 |
A" |
233 |
233 |
1.27 |
3.95 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8249.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8249.3 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 wB97X-D/LANL2DZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.003 |
-1.894 |
0.000 |
C2 |
0.000 |
-0.565 |
0.000 |
C3 |
-0.001 |
0.718 |
0.000 |
O4 |
-0.002 |
1.922 |
0.000 |
H5 |
0.932 |
-2.465 |
0.000 |
H6 |
-0.923 |
-2.469 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
C1 | | 1.3287 | 2.6117 | 3.8153 | 1.0903 | 1.0902 |
C2 | 1.3287 | | 1.2830 | 2.4866 | 2.1160 | 2.1161 | C3 | 2.6117 | 1.2830 | | 1.2036 | 3.3168 | 3.3178 | O4 | 3.8153 | 2.4866 | 1.2036 | | 4.4849 | 4.4863 | H5 | 1.0903 | 2.1160 | 3.3168 | 4.4849 | | 1.8547 | H6 | 1.0902 | 2.1161 | 3.3178 | 4.4863 | 1.8547 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
179.922 |
|
C2 |
C1 |
H5 |
121.722 |
C2 |
C1 |
H6 |
121.730 |
|
C2 |
C3 |
O4 |
179.990 |
H5 |
C1 |
H6 |
116.548 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.411 |
|
|
|
2 |
C |
-0.130 |
|
|
|
3 |
C |
0.256 |
|
|
|
4 |
O |
-0.187 |
|
|
|
5 |
H |
0.236 |
|
|
|
6 |
H |
0.236 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.007 |
-3.389 |
0.000 |
3.389 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.330 |
-0.004 |
0.000 |
y |
-0.004 |
-22.195 |
0.000 |
z |
0.000 |
0.000 |
-22.791 |
|
Traceless |
| x | y | z |
x |
0.163 |
-0.004 |
0.000 |
y |
-0.004 |
0.365 |
0.000 |
z |
0.000 |
0.000 |
-0.528 |
|
Polar |
3z2-r2 | -1.056 |
x2-y2 | -0.135 |
xy | -0.004 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.514 |
-0.012 |
0.000 |
y |
-0.012 |
10.734 |
0.000 |
z |
0.000 |
0.000 |
1.849 |
<r2> (average value of r
2) Å
2
<r2> |
83.974 |
(<r2>)1/2 |
9.164 |