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S1C2
Vibrational Frequencies calculated at HF/TZVP
Geometric Data calculated at HF/TZVP
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at HF/TZVP
| hartrees |
Energy at 0K | -206.844485 |
Energy at 298.15K | -206.848045 |
HF Energy | -206.844485 |
Nuclear repulsion energy | 103.351067 |
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/TZVP
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 |
4148 |
3769 |
77.09 |
53.90 |
0.26 |
0.41 |
2 |
A |
3283 |
2983 |
6.69 |
71.35 |
0.42 |
0.59 |
3 |
A |
3206 |
2913 |
26.10 |
109.55 |
0.12 |
0.21 |
4 |
A |
2605 |
2367 |
1.55 |
56.24 |
0.17 |
0.29 |
5 |
A |
1621 |
1473 |
2.85 |
8.77 |
0.71 |
0.83 |
6 |
A |
1543 |
1402 |
60.27 |
3.07 |
0.73 |
0.84 |
7 |
A |
1491 |
1355 |
6.83 |
5.06 |
0.74 |
0.85 |
8 |
A |
1319 |
1198 |
25.13 |
2.05 |
0.64 |
0.78 |
9 |
A |
1204 |
1094 |
122.77 |
8.00 |
0.36 |
0.52 |
10 |
A |
1080 |
981 |
28.69 |
0.37 |
0.63 |
0.78 |
11 |
A |
945 |
858 |
31.60 |
2.51 |
0.14 |
0.25 |
12 |
A |
637 |
579 |
0.91 |
2.78 |
0.30 |
0.46 |
13 |
A |
421 |
382 |
41.93 |
2.58 |
0.74 |
0.85 |
14 |
A |
336 |
305 |
142.89 |
3.80 |
0.74 |
0.85 |
15 |
A |
245 |
223 |
15.11 |
5.41 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12041.9 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 10941.2 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/TZVP
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.570 |
0.581 |
0.037 |
C2 |
0.830 |
0.096 |
-0.005 |
O3 |
-1.498 |
-0.440 |
-0.110 |
H4 |
-0.699 |
1.128 |
0.965 |
H5 |
-0.711 |
1.269 |
-0.783 |
H6 |
-1.437 |
-1.051 |
0.605 |
N7 |
1.895 |
-0.270 |
-0.014 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4818 | 1.3877 | 1.0841 | 1.0792 | 1.9337 | 2.6084 |
C2 | 1.4818 | | 2.3905 | 2.0833 | 2.0870 | 2.6125 | 1.1267 | O3 | 1.3877 | 2.3905 | | 2.0616 | 1.9977 | 0.9428 | 3.3985 | H4 | 1.0841 | 2.0833 | 2.0616 | | 1.7530 | 2.3280 | 3.1050 | H5 | 1.0792 | 2.0870 | 1.9977 | 1.7530 | | 2.7991 | 3.1229 | H6 | 1.9337 | 2.6125 | 0.9428 | 2.3280 | 2.7991 | | 3.4782 | N7 | 2.6084 | 1.1267 | 3.3985 | 3.1050 | 3.1229 | 3.4782 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
178.866 |
|
C1 |
O3 |
H6 |
110.693 |
C2 |
C1 |
O3 |
112.791 |
|
C2 |
C1 |
H4 |
107.555 |
C2 |
C1 |
H5 |
108.129 |
|
O3 |
C1 |
H4 |
112.453 |
O3 |
C1 |
H5 |
107.492 |
|
H4 |
C1 |
H5 |
108.258 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/TZVP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.041 |
|
|
|
2 |
C |
-0.037 |
|
|
|
3 |
O |
-0.408 |
|
|
|
4 |
H |
0.116 |
|
|
|
5 |
H |
0.128 |
|
|
|
6 |
H |
0.288 |
|
|
|
7 |
N |
-0.129 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.574 |
1.299 |
1.486 |
3.244 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-32.868 |
1.239 |
-2.234 |
y |
1.239 |
-20.751 |
-1.856 |
z |
-2.234 |
-1.856 |
-21.932 |
|
Traceless |
| x | y | z |
x |
-11.527 |
1.239 |
-2.234 |
y |
1.239 |
6.649 |
-1.856 |
z |
-2.234 |
-1.856 |
4.878 |
|
Polar |
3z2-r2 | 9.755 |
x2-y2 | -12.117 |
xy | 1.239 |
xz | -2.234 |
yz | -1.856 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.340 |
-0.455 |
-0.041 |
y |
-0.455 |
3.616 |
-0.088 |
z |
-0.041 |
-0.088 |
3.178 |
<r2> (average value of r
2) Å
2
<r2> |
78.097 |
(<r2>)1/2 |
8.837 |