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S1C2
Vibrational Frequencies calculated at HF/CEP-121G*
Geometric Data calculated at HF/CEP-121G*
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at HF/CEP-121G*
| hartrees |
Energy at 0K | -38.082828 |
Energy at 298.15K | -38.086356 |
HF Energy | -38.082828 |
Nuclear repulsion energy | 55.422959 |
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/CEP-121G*
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 |
4129 |
3730 |
59.14 |
56.24 |
0.30 |
0.46 |
2 |
A |
3324 |
3003 |
12.62 |
69.82 |
0.46 |
0.63 |
3 |
A |
3241 |
2927 |
36.59 |
108.97 |
0.12 |
0.21 |
4 |
A |
2559 |
2312 |
1.36 |
54.64 |
0.17 |
0.29 |
5 |
A |
1632 |
1474 |
0.96 |
9.80 |
0.72 |
0.84 |
6 |
A |
1546 |
1397 |
84.84 |
4.22 |
0.71 |
0.83 |
7 |
A |
1494 |
1349 |
5.94 |
5.30 |
0.74 |
0.85 |
8 |
A |
1322 |
1194 |
30.55 |
2.14 |
0.70 |
0.82 |
9 |
A |
1208 |
1092 |
123.19 |
9.26 |
0.35 |
0.52 |
10 |
A |
1077 |
973 |
28.69 |
0.43 |
0.55 |
0.71 |
11 |
A |
937 |
847 |
36.69 |
3.42 |
0.13 |
0.23 |
12 |
A |
627 |
567 |
1.20 |
2.72 |
0.30 |
0.46 |
13 |
A |
417 |
377 |
49.96 |
2.13 |
0.75 |
0.85 |
14 |
A |
334 |
302 |
141.55 |
4.25 |
0.75 |
0.85 |
15 |
A |
240 |
217 |
15.63 |
5.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12043.0 cm
-1
Scaled (by 0.9034) Zero Point Vibrational Energy (zpe) 10879.7 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/CEP-121G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.579 |
0.588 |
0.037 |
C2 |
0.836 |
0.098 |
-0.006 |
O3 |
-1.506 |
-0.447 |
-0.112 |
H4 |
-0.710 |
1.131 |
0.968 |
H5 |
-0.724 |
1.273 |
-0.786 |
H6 |
-1.441 |
-1.050 |
0.616 |
N7 |
1.911 |
-0.271 |
-0.013 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4980 | 1.3972 | 1.0858 | 1.0809 | 1.9396 | 2.6348 |
C2 | 1.4980 | | 2.4071 | 2.0990 | 2.1032 | 2.6252 | 1.1370 | O3 | 1.3972 | 2.4071 | | 2.0713 | 2.0062 | 0.9480 | 3.4235 | H4 | 1.0858 | 2.0990 | 2.0713 | | 1.7598 | 2.3274 | 3.1306 | H5 | 1.0809 | 2.1032 | 2.0062 | 1.7598 | | 2.8071 | 3.1508 | H6 | 1.9396 | 2.6252 | 0.9480 | 2.3274 | 2.8071 | | 3.4990 | N7 | 2.6348 | 1.1370 | 3.4235 | 3.1306 | 3.1508 | 3.4990 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
178.711 |
|
C1 |
O3 |
H6 |
110.113 |
C2 |
C1 |
O3 |
112.441 |
|
C2 |
C1 |
H4 |
107.587 |
C2 |
C1 |
H5 |
108.188 |
|
O3 |
C1 |
H4 |
112.453 |
O3 |
C1 |
H5 |
107.417 |
|
H4 |
C1 |
H5 |
108.623 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/CEP-121G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.047 |
|
|
|
2 |
C |
-0.099 |
|
|
|
3 |
O |
-0.623 |
|
|
|
4 |
H |
0.190 |
|
|
|
5 |
H |
0.208 |
|
|
|
6 |
H |
0.451 |
|
|
|
7 |
N |
-0.081 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.592 |
1.306 |
1.532 |
3.282 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.698 |
1.185 |
-2.295 |
y |
1.185 |
-20.630 |
-1.929 |
z |
-2.295 |
-1.929 |
-21.790 |
|
Traceless |
| x | y | z |
x |
-11.488 |
1.185 |
-2.295 |
y |
1.185 |
6.614 |
-1.929 |
z |
-2.295 |
-1.929 |
4.873 |
|
Polar |
3z2-r2 | 9.747 |
x2-y2 | -12.068 |
xy | 1.185 |
xz | -2.295 |
yz | -1.929 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.154 |
-0.432 |
-0.032 |
y |
-0.432 |
3.540 |
-0.110 |
z |
-0.032 |
-0.110 |
3.120 |
<r2> (average value of r
2) Å
2
<r2> |
63.765 |
(<r2>)1/2 |
7.985 |