Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -190.578160 |
| Energy at 298.15K | |
| HF Energy | -190.578160 |
| Nuclear repulsion energy | 88.394263 |
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 B1B95/6-31G*
| 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 |
3123 |
2965 |
28.24 |
191.73 |
0.11 |
0.20 |
| 2 |
A1 |
2375 |
2255 |
888.46 |
30.30 |
0.35 |
0.51 |
| 3 |
A1 |
1839 |
1746 |
25.09 |
0.66 |
0.53 |
0.70 |
| 4 |
A1 |
1503 |
1427 |
4.68 |
17.70 |
0.53 |
0.69 |
| 5 |
A1 |
948 |
900 |
6.35 |
39.29 |
0.28 |
0.44 |
| 6 |
B1 |
1020 |
968 |
24.34 |
0.08 |
0.75 |
0.86 |
| 7 |
B1 |
657 |
624 |
22.38 |
2.26 |
0.75 |
0.86 |
| 8 |
B1 |
236 |
224 |
0.01 |
4.59 |
0.75 |
0.86 |
| 9 |
B2 |
3194 |
3032 |
12.73 |
126.24 |
0.75 |
0.86 |
| 10 |
B2 |
1075 |
1020 |
1.20 |
0.35 |
0.75 |
0.86 |
| 11 |
B2 |
454 |
431 |
16.38 |
1.87 |
0.75 |
0.86 |
| 12 |
B2 |
67i |
64i |
15.12 |
0.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8178.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 7763.3 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 B1B95/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.872 |
| C2 |
0.000 |
0.000 |
-0.557 |
| C3 |
0.000 |
0.000 |
0.719 |
| O4 |
0.000 |
0.000 |
1.896 |
| H5 |
0.000 |
0.923 |
-2.453 |
| H6 |
0.000 |
-0.923 |
-2.453 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3145 | 2.5909 | 3.7679 | 1.0904 | 1.0904 |
C2 | 1.3145 | | 1.2764 | 2.4534 | 2.1082 | 2.1082 | C3 | 2.5909 | 1.2764 | | 1.1770 | 3.3035 | 3.3035 | O4 | 3.7679 | 2.4534 | 1.1770 | | 4.4459 | 4.4459 | H5 | 1.0904 | 2.1082 | 3.3035 | 4.4459 | | 1.8451 | H6 | 1.0904 | 2.1082 | 3.3035 | 4.4459 | 1.8451 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
122.209 |
| C2 |
C1 |
H6 |
122.209 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
115.581 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.445 |
|
|
|
| 2 |
C |
0.263 |
|
|
|
| 3 |
C |
0.177 |
|
|
|
| 4 |
O |
-0.389 |
|
|
|
| 5 |
H |
0.197 |
|
|
|
| 6 |
H |
0.197 |
|
|
|
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 |
-2.694 |
2.694 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.077 |
0.000 |
0.000 |
| y |
0.000 |
-21.883 |
0.000 |
| z |
0.000 |
0.000 |
-21.349 |
|
| Traceless |
| | x | y | z |
| x |
-0.461 |
0.000 |
0.000 |
| y |
0.000 |
-0.170 |
0.000 |
| z |
0.000 |
0.000 |
0.631 |
|
| Polar |
| 3z2-r2 | 1.262 |
| x2-y2 | -0.194 |
| 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 |
1.852 |
0.000 |
0.000 |
| y |
0.000 |
2.719 |
0.000 |
| z |
0.000 |
0.000 |
10.054 |
<r2> (average value of r
2) Å
2
| <r2> |
82.084 |
| (<r2>)1/2 |
9.060 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -190.578465 |
| Energy at 298.15K | |
| HF Energy | -190.578465 |
| Nuclear repulsion energy | 88.535472 |
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 B1B95/6-31G*
| 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' |
3206 |
3044 |
12.66 |
120.07 |
0.69 |
0.82 |
| 2 |
A' |
3130 |
2971 |
27.26 |
159.43 |
0.12 |
0.21 |
| 3 |
A' |
2303 |
2187 |
895.42 |
34.42 |
0.36 |
0.53 |
| 4 |
A' |
1819 |
1726 |
11.09 |
1.01 |
0.66 |
0.80 |
| 5 |
A' |
1507 |
1431 |
2.15 |
18.72 |
0.55 |
0.71 |
| 6 |
A' |
1076 |
1021 |
11.73 |
4.05 |
0.16 |
0.28 |
| 7 |
A' |
966 |
917 |
4.06 |
33.57 |
0.23 |
0.37 |
| 8 |
A' |
484 |
460 |
15.88 |
3.78 |
0.61 |
0.76 |
| 9 |
A' |
127 |
121 |
19.77 |
4.86 |
0.74 |
0.85 |
| 10 |
A" |
1025 |
973 |
24.07 |
0.17 |
0.75 |
0.86 |
| 11 |
A" |
691 |
656 |
17.89 |
2.72 |
0.75 |
0.86 |
| 12 |
A" |
261 |
247 |
1.52 |
6.18 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8296.7 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 7876.1 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.866 |
-1.620 |
0.000 |
| C2 |
0.000 |
-0.623 |
0.000 |
| C3 |
-0.291 |
0.637 |
0.000 |
| O4 |
-0.742 |
1.720 |
0.000 |
| H5 |
1.946 |
-1.468 |
0.000 |
| H6 |
0.539 |
-2.658 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3210 | 2.5369 | 3.7071 | 1.0906 | 1.0887 |
C2 | 1.3210 | | 1.2934 | 2.4575 | 2.1221 | 2.1054 | C3 | 2.5369 | 1.2934 | | 1.1728 | 3.0724 | 3.3984 | O4 | 3.7071 | 2.4575 | 1.1728 | | 4.1704 | 4.5616 | H5 | 1.0906 | 2.1221 | 3.0724 | 4.1704 | | 1.8433 | H6 | 1.0887 | 2.1054 | 3.3984 | 4.5616 | 1.8433 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
152.017 |
|
C2 |
C1 |
H5 |
122.986 |
| C2 |
C1 |
H6 |
121.486 |
|
C2 |
C3 |
O4 |
170.384 |
| H5 |
C1 |
H6 |
115.527 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.374 |
|
|
|
| 2 |
C |
0.022 |
|
|
|
| 3 |
C |
0.338 |
|
|
|
| 4 |
O |
-0.373 |
|
|
|
| 5 |
H |
0.195 |
|
|
|
| 6 |
H |
0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.634 |
-1.910 |
0.000 |
2.514 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.464 |
-0.772 |
0.000 |
| y |
-0.772 |
-22.022 |
0.000 |
| z |
0.000 |
0.000 |
-22.160 |
|
| Traceless |
| | x | y | z |
| x |
0.627 |
-0.772 |
0.000 |
| y |
-0.772 |
-0.210 |
0.000 |
| z |
0.000 |
0.000 |
-0.417 |
|
| Polar |
| 3z2-r2 | -0.834 |
| x2-y2 | 0.558 |
| xy | -0.772 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.221 |
-2.555 |
0.000 |
| y |
-2.555 |
8.578 |
0.000 |
| z |
0.000 |
0.000 |
1.897 |
<r2> (average value of r
2) Å
2
| <r2> |
80.563 |
| (<r2>)1/2 |
8.976 |