Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -153.422887 |
| Energy at 298.15K | |
| HF Energy | -153.422887 |
| Nuclear repulsion energy | 74.018398 |
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 B1B95/3-21G
| 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' |
3501 |
3350 |
2.39 |
|
|
|
| 2 |
A' |
3184 |
3046 |
7.90 |
|
|
|
| 3 |
A' |
3022 |
2891 |
50.99 |
|
|
|
| 4 |
A' |
1586 |
1518 |
1.54 |
|
|
|
| 5 |
A' |
1507 |
1442 |
1.54 |
|
|
|
| 6 |
A' |
1458 |
1395 |
3.37 |
|
|
|
| 7 |
A' |
1256 |
1202 |
45.72 |
|
|
|
| 8 |
A' |
1025 |
981 |
20.30 |
|
|
|
| 9 |
A' |
953 |
912 |
67.42 |
|
|
|
| 10 |
A' |
628 |
601 |
30.28 |
|
|
|
| 11 |
A' |
350 |
335 |
34.83 |
|
|
|
| 12 |
A" |
3296 |
3153 |
11.89 |
|
|
|
| 13 |
A" |
3054 |
2922 |
59.95 |
|
|
|
| 14 |
A" |
1315 |
1258 |
0.06 |
|
|
|
| 15 |
A" |
1169 |
1118 |
0.52 |
|
|
|
| 16 |
A" |
842 |
806 |
0.02 |
|
|
|
| 17 |
A" |
252 |
241 |
148.33 |
|
|
|
| 18 |
A" |
135i |
129i |
1.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14131.8 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 13519.9 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.110 |
-0.410 |
0.000 |
| C2 |
0.000 |
0.556 |
0.000 |
| C3 |
1.266 |
-0.223 |
0.000 |
| H4 |
-1.948 |
0.121 |
0.000 |
| H5 |
-0.038 |
1.201 |
0.887 |
| H6 |
-0.038 |
1.201 |
-0.887 |
| H7 |
1.653 |
-0.621 |
-0.929 |
| H8 |
1.653 |
-0.621 |
0.929 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4714 | 2.3830 | 0.9925 | 2.1288 | 2.1288 | 2.9221 | 2.9221 |
C2 | 1.4714 | | 1.4865 | 1.9961 | 1.0978 | 1.0978 | 2.2314 | 2.2314 | C3 | 2.3830 | 1.4865 | | 3.2324 | 2.1253 | 2.1253 | 1.0818 | 1.0818 | H4 | 0.9925 | 1.9961 | 3.2324 | | 2.3667 | 2.3667 | 3.7920 | 3.7920 | H5 | 2.1288 | 1.0978 | 2.1253 | 2.3667 | | 1.7747 | 3.0785 | 2.4863 | H6 | 2.1288 | 1.0978 | 2.1253 | 2.3667 | 1.7747 | | 2.4863 | 3.0785 | H7 | 2.9221 | 2.2314 | 1.0818 | 3.7920 | 3.0785 | 2.4863 | | 1.8571 | H8 | 2.9221 | 2.2314 | 1.0818 | 3.7920 | 2.4863 | 3.0785 | 1.8571 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
107.346 |
|
O1 |
C2 |
H5 |
111.075 |
| O1 |
C2 |
H6 |
111.075 |
|
C2 |
O1 |
H4 |
106.598 |
| C2 |
C3 |
H7 |
119.827 |
|
C2 |
C3 |
H8 |
119.827 |
| C3 |
C2 |
H5 |
109.738 |
|
C3 |
C2 |
H6 |
109.738 |
| H5 |
C2 |
H6 |
107.869 |
|
H7 |
C3 |
H8 |
118.270 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.553 |
|
|
|
| 2 |
C |
-0.249 |
|
|
|
| 3 |
C |
-0.360 |
|
|
|
| 4 |
H |
0.340 |
|
|
|
| 5 |
H |
0.198 |
|
|
|
| 6 |
H |
0.198 |
|
|
|
| 7 |
H |
0.213 |
|
|
|
| 8 |
H |
0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.215 |
1.654 |
0.000 |
1.668 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.160 |
-2.922 |
0.000 |
| y |
-2.922 |
-19.864 |
0.000 |
| z |
0.000 |
0.000 |
-18.501 |
|
| Traceless |
| | x | y | z |
| x |
3.023 |
-2.922 |
0.000 |
| y |
-2.922 |
-2.534 |
0.000 |
| z |
0.000 |
0.000 |
-0.489 |
|
| Polar |
| 3z2-r2 | -0.978 |
| x2-y2 | 3.705 |
| xy | -2.922 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.064 |
-0.532 |
0.000 |
| y |
-0.532 |
2.870 |
0.000 |
| z |
0.000 |
0.000 |
3.054 |
<r2> (average value of r
2) Å
2
| <r2> |
50.551 |
| (<r2>)1/2 |
7.110 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -153.424879 |
| Energy at 298.15K | -153.429410 |
| HF Energy | -153.424879 |
| Nuclear repulsion energy | 74.458601 |
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 B1B95/3-21G
| 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 |
3556 |
3402 |
0.73 |
|
|
|
| 2 |
A |
3325 |
3181 |
4.09 |
|
|
|
| 3 |
A |
3201 |
3062 |
4.71 |
|
|
|
| 4 |
A |
2968 |
2840 |
61.07 |
|
|
|
| 5 |
A |
2920 |
2794 |
61.61 |
|
|
|
| 6 |
A |
1560 |
1492 |
4.66 |
|
|
|
| 7 |
A |
1475 |
1411 |
4.93 |
|
|
|
| 8 |
A |
1453 |
1390 |
0.18 |
|
|
|
| 9 |
A |
1280 |
1225 |
56.21 |
|
|
|
| 10 |
A |
1219 |
1166 |
2.08 |
|
|
|
| 11 |
A |
1099 |
1051 |
20.21 |
|
|
|
| 12 |
A |
1054 |
1008 |
36.39 |
|
|
|
| 13 |
A |
974 |
932 |
6.08 |
|
|
|
| 14 |
A |
876 |
838 |
19.45 |
|
|
|
| 15 |
A |
419 |
401 |
30.21 |
|
|
|
| 16 |
A |
389 |
372 |
79.34 |
|
|
|
| 17 |
A |
284 |
272 |
98.66 |
|
|
|
| 18 |
A |
100 |
96 |
29.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14075.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 13466.1 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 B1B95/3-21G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-1.117 |
-0.377 |
-0.056 |
| C2 |
0.004 |
0.536 |
0.032 |
| C3 |
1.243 |
-0.269 |
-0.015 |
| H4 |
-1.946 |
0.129 |
0.106 |
| H5 |
-0.016 |
1.122 |
0.972 |
| H6 |
0.021 |
1.278 |
-0.784 |
| H7 |
2.195 |
0.201 |
-0.217 |
| H8 |
1.200 |
-1.310 |
0.271 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| O1 | | 1.4482 | 2.3630 | 0.9851 | 2.1255 | 2.1368 | 3.3662 | 2.5187 |
C2 | 1.4482 | | 1.4785 | 1.9935 | 1.1086 | 1.1033 | 2.2309 | 2.2120 | C3 | 2.3630 | 1.4785 | | 3.2165 | 2.1205 | 2.1164 | 1.0810 | 1.0799 | H4 | 0.9851 | 1.9935 | 3.2165 | | 2.3371 | 2.4463 | 4.1549 | 3.4634 | H5 | 2.1255 | 1.1086 | 2.1205 | 2.3371 | | 1.7638 | 2.6748 | 2.8078 | H6 | 2.1368 | 1.1033 | 2.1164 | 2.4463 | 1.7638 | | 2.4916 | 3.0330 | H7 | 3.3662 | 2.2309 | 1.0810 | 4.1549 | 2.6748 | 2.4916 | | 1.8738 | H8 | 2.5187 | 2.2120 | 1.0799 | 3.4634 | 2.8078 | 3.0330 | 1.8738 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C2 |
C3 |
107.676 |
|
O1 |
C2 |
H5 |
111.778 |
| O1 |
C2 |
H6 |
113.055 |
|
C2 |
O1 |
H4 |
108.515 |
| C2 |
C3 |
H7 |
120.497 |
|
C2 |
C3 |
H8 |
118.847 |
| C3 |
C2 |
H5 |
109.265 |
|
C3 |
C2 |
H6 |
109.252 |
| H5 |
C2 |
H6 |
105.763 |
|
H7 |
C3 |
H8 |
120.260 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.570 |
|
|
|
| 2 |
C |
-0.224 |
|
|
|
| 3 |
C |
-0.385 |
|
|
|
| 4 |
H |
0.347 |
|
|
|
| 5 |
H |
0.201 |
|
|
|
| 6 |
H |
0.202 |
|
|
|
| 7 |
H |
0.198 |
|
|
|
| 8 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.315 |
1.853 |
0.346 |
1.911 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.425 |
-1.971 |
-0.372 |
| y |
-1.971 |
-18.792 |
-0.334 |
| z |
-0.372 |
-0.334 |
-20.147 |
|
| Traceless |
| | x | y | z |
| x |
4.045 |
-1.971 |
-0.372 |
| y |
-1.971 |
-1.006 |
-0.334 |
| z |
-0.372 |
-0.334 |
-3.039 |
|
| Polar |
| 3z2-r2 | -6.078 |
| x2-y2 | 3.367 |
| xy | -1.971 |
| xz | -0.372 |
| yz | -0.334 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.217 |
-0.196 |
-0.148 |
| y |
-0.196 |
3.483 |
-0.088 |
| z |
-0.148 |
-0.088 |
2.236 |
<r2> (average value of r
2) Å
2
| <r2> |
50.281 |
| (<r2>)1/2 |
7.091 |