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S1C2
Vibrational Frequencies calculated at HF/3-21G*
Geometric Data calculated at HF/3-21G*
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -205.612263 |
Energy at 298.15K | -205.615916 |
HF Energy | -205.612263 |
Nuclear repulsion energy | 102.308511 |
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 HF/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 |
3864 |
3488 |
29.47 |
81.59 |
0.32 |
0.49 |
2 |
A |
3307 |
2985 |
4.10 |
79.32 |
0.45 |
0.62 |
3 |
A |
3229 |
2914 |
20.26 |
96.54 |
0.17 |
0.29 |
4 |
A |
2593 |
2340 |
0.05 |
31.53 |
0.26 |
0.41 |
5 |
A |
1670 |
1507 |
4.26 |
18.83 |
0.70 |
0.82 |
6 |
A |
1530 |
1381 |
14.37 |
8.68 |
0.69 |
0.82 |
7 |
A |
1497 |
1351 |
14.21 |
12.02 |
0.75 |
0.86 |
8 |
A |
1364 |
1231 |
30.21 |
3.71 |
0.73 |
0.84 |
9 |
A |
1123 |
1014 |
41.84 |
12.60 |
0.36 |
0.53 |
10 |
A |
1075 |
971 |
79.56 |
1.58 |
0.53 |
0.69 |
11 |
A |
949 |
857 |
41.80 |
2.34 |
0.10 |
0.19 |
12 |
A |
662 |
597 |
1.25 |
2.62 |
0.30 |
0.46 |
13 |
A |
488 |
440 |
23.67 |
2.99 |
0.74 |
0.85 |
14 |
A |
355 |
321 |
195.95 |
7.64 |
0.75 |
0.86 |
15 |
A |
261 |
236 |
8.04 |
5.36 |
0.74 |
0.85 |
Unscaled Zero Point Vibrational Energy (zpe) 11982.9 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 10815.8 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 HF/3-21G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.552 |
0.604 |
0.037 |
C2 |
0.831 |
0.112 |
0.003 |
O3 |
-1.509 |
-0.452 |
-0.113 |
H4 |
-0.698 |
1.163 |
0.953 |
H5 |
-0.711 |
1.269 |
-0.797 |
H6 |
-1.463 |
-1.067 |
0.632 |
N7 |
1.896 |
-0.291 |
-0.017 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4683 | 1.4333 | 1.0831 | 1.0781 | 1.9947 | 2.6066 |
C2 | 1.4683 | | 2.4102 | 2.0849 | 2.0872 | 2.6555 | 1.1384 | O3 | 1.4333 | 2.4102 | | 2.0981 | 2.0166 | 0.9671 | 3.4101 | H4 | 1.0831 | 2.0849 | 2.0981 | | 1.7527 | 2.3798 | 3.1279 | H5 | 1.0781 | 2.0872 | 2.0166 | 1.7527 | | 2.8399 | 3.1364 | H6 | 1.9947 | 2.6555 | 0.9671 | 2.3798 | 2.8399 | | 3.5081 | N7 | 2.6066 | 1.1384 | 3.4101 | 3.1279 | 3.1364 | 3.5081 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
178.802 |
|
C1 |
O3 |
H6 |
110.896 |
C2 |
C1 |
O3 |
112.323 |
|
C2 |
C1 |
H4 |
108.660 |
C2 |
C1 |
H5 |
109.141 |
|
O3 |
C1 |
H4 |
112.230 |
O3 |
C1 |
H5 |
105.965 |
|
H4 |
C1 |
H5 |
108.393 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.087 |
|
|
|
2 |
C |
0.294 |
|
|
|
3 |
O |
-0.650 |
|
|
|
4 |
H |
0.250 |
|
|
|
5 |
H |
0.291 |
|
|
|
6 |
H |
0.393 |
|
|
|
7 |
N |
-0.492 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.112 |
1.375 |
1.664 |
3.020 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.665 |
1.267 |
-2.499 |
y |
1.267 |
-20.482 |
-1.921 |
z |
-2.499 |
-1.921 |
-21.736 |
|
Traceless |
| x | y | z |
x |
-11.556 |
1.267 |
-2.499 |
y |
1.267 |
6.719 |
-1.921 |
z |
-2.499 |
-1.921 |
4.837 |
|
Polar |
3z2-r2 | 9.675 |
x2-y2 | -12.183 |
xy | 1.267 |
xz | -2.499 |
yz | -1.921 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.378 |
-0.361 |
-0.059 |
y |
-0.361 |
2.973 |
-0.204 |
z |
-0.059 |
-0.204 |
2.496 |
<r2> (average value of r
2) Å
2
<r2> |
78.724 |
(<r2>)1/2 |
8.873 |