Jump to
S1C2
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -189.493339 |
| Energy at 298.15K | |
| HF Energy | -189.493339 |
| Nuclear repulsion energy | 87.386157 |
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 B97D3/3-21G*
| 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 |
3010 |
3010 |
32.69 |
184.99 |
0.11 |
0.20 |
| 2 |
A1 |
2276 |
2276 |
516.05 |
15.29 |
0.36 |
0.53 |
| 3 |
A1 |
1725 |
1725 |
16.84 |
2.33 |
0.51 |
0.67 |
| 4 |
A1 |
1501 |
1501 |
5.29 |
20.80 |
0.54 |
0.70 |
| 5 |
A1 |
906 |
906 |
6.36 |
33.93 |
0.30 |
0.46 |
| 6 |
B1 |
987 |
987 |
27.57 |
0.15 |
0.75 |
0.86 |
| 7 |
B1 |
751 |
751 |
20.38 |
2.95 |
0.75 |
0.86 |
| 8 |
B1 |
234 |
234 |
0.71 |
4.99 |
0.75 |
0.86 |
| 9 |
B2 |
3070 |
3070 |
20.94 |
130.65 |
0.75 |
0.86 |
| 10 |
B2 |
1080 |
1080 |
0.45 |
0.16 |
0.75 |
0.86 |
| 11 |
B2 |
512 |
512 |
14.95 |
1.32 |
0.75 |
0.86 |
| 12 |
B2 |
52i |
52i |
14.54 |
0.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 7999.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7999.4 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 B97D3/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.887 |
| C2 |
0.000 |
0.000 |
-0.564 |
| C3 |
0.000 |
0.000 |
0.713 |
| O4 |
0.000 |
0.000 |
1.922 |
| H5 |
0.000 |
0.928 |
-2.473 |
| H6 |
0.000 |
-0.928 |
-2.473 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3228 | 2.5996 | 3.8095 | 1.0977 | 1.0977 |
C2 | 1.3228 | | 1.2768 | 2.4867 | 2.1225 | 2.1225 | C3 | 2.5996 | 1.2768 | | 1.2099 | 3.3181 | 3.3181 | O4 | 3.8095 | 2.4867 | 1.2099 | | 4.4925 | 4.4925 | H5 | 1.0977 | 2.1225 | 3.3181 | 4.4925 | | 1.8564 | H6 | 1.0977 | 2.1225 | 3.3181 | 4.4925 | 1.8564 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
122.266 |
| C2 |
C1 |
H6 |
122.266 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
115.468 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.375 |
|
|
|
| 2 |
C |
0.194 |
|
|
|
| 3 |
C |
0.160 |
|
|
|
| 4 |
O |
-0.441 |
|
|
|
| 5 |
H |
0.230 |
|
|
|
| 6 |
H |
0.230 |
|
|
|
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 |
-2.661 |
2.661 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.486 |
0.000 |
0.000 |
| y |
0.000 |
-22.256 |
0.000 |
| z |
0.000 |
0.000 |
-21.347 |
|
| Traceless |
| | x | y | z |
| x |
-0.684 |
0.000 |
0.000 |
| y |
0.000 |
-0.340 |
0.000 |
| z |
0.000 |
0.000 |
1.024 |
|
| Polar |
| 3z2-r2 | 2.047 |
| x2-y2 | -0.229 |
| 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 |
1.398 |
0.000 |
0.000 |
| y |
0.000 |
2.296 |
0.000 |
| z |
0.000 |
0.000 |
9.741 |
<r2> (average value of r
2) Å
2
| <r2> |
83.604 |
| (<r2>)1/2 |
9.144 |
Jump to
S1C1
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -189.493384 |
| Energy at 298.15K | |
| HF Energy | -189.493384 |
| Nuclear repulsion energy | 87.453901 |
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 B97D3/3-21G*
| 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' |
3080 |
3080 |
20.56 |
130.55 |
0.70 |
0.82 |
| 2 |
A' |
3015 |
3015 |
32.20 |
173.28 |
0.12 |
0.21 |
| 3 |
A' |
2254 |
2254 |
517.18 |
16.50 |
0.37 |
0.55 |
| 4 |
A' |
1723 |
1723 |
15.26 |
2.05 |
0.56 |
0.72 |
| 5 |
A' |
1506 |
1506 |
4.52 |
20.99 |
0.55 |
0.71 |
| 6 |
A' |
1086 |
1086 |
3.12 |
1.26 |
0.23 |
0.37 |
| 7 |
A' |
914 |
914 |
5.74 |
32.02 |
0.28 |
0.44 |
| 8 |
A' |
501 |
501 |
13.58 |
2.13 |
0.67 |
0.80 |
| 9 |
A' |
82 |
82 |
16.15 |
2.15 |
0.74 |
0.85 |
| 10 |
A" |
995 |
995 |
28.36 |
0.22 |
0.75 |
0.86 |
| 11 |
A" |
743 |
743 |
18.24 |
3.20 |
0.75 |
0.86 |
| 12 |
A" |
249 |
249 |
0.06 |
5.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8073.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8073.6 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 B97D3/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.543 |
-1.795 |
0.000 |
| C2 |
0.000 |
-0.587 |
0.000 |
| C3 |
-0.192 |
0.680 |
0.000 |
| O4 |
-0.458 |
1.859 |
0.000 |
| H5 |
1.629 |
-1.956 |
0.000 |
| H6 |
-0.069 |
-2.705 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3247 | 2.5820 | 3.7884 | 1.0980 | 1.0961 |
C2 | 1.3247 | | 1.2813 | 2.4879 | 2.1280 | 2.1194 | C3 | 2.5820 | 1.2813 | | 1.2083 | 3.2040 | 3.3873 | O4 | 3.7884 | 2.4879 | 1.2083 | | 4.3484 | 4.5803 | H5 | 1.0980 | 2.1280 | 3.2040 | 4.3484 | | 1.8552 | H6 | 1.0961 | 2.1194 | 3.3873 | 4.5803 | 1.8552 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
164.441 |
|
C2 |
C1 |
H5 |
122.618 |
| C2 |
C1 |
H6 |
121.919 |
|
C2 |
C3 |
O4 |
175.906 |
| H5 |
C1 |
H6 |
115.463 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.398 |
|
|
|
| 2 |
C |
0.158 |
|
|
|
| 3 |
C |
0.215 |
|
|
|
| 4 |
O |
-0.434 |
|
|
|
| 5 |
H |
0.228 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.041 |
-2.388 |
0.000 |
2.605 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.025 |
-0.713 |
0.000 |
| y |
-0.713 |
-21.712 |
0.000 |
| z |
0.000 |
0.000 |
-22.504 |
|
| Traceless |
| | x | y | z |
| x |
0.083 |
-0.713 |
0.000 |
| y |
-0.713 |
0.553 |
0.000 |
| z |
0.000 |
0.000 |
-0.636 |
|
| Polar |
| 3z2-r2 | -1.272 |
| x2-y2 | -0.313 |
| xy | -0.713 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.886 |
-1.801 |
0.000 |
| y |
-1.801 |
9.148 |
0.000 |
| z |
0.000 |
0.000 |
1.413 |
<r2> (average value of r
2) Å
2
| <r2> |
83.074 |
| (<r2>)1/2 |
9.114 |