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S1C2
Vibrational Frequencies calculated at B3LYP/6-31G**
Geometric Data calculated at B3LYP/6-31G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B3LYP/6-31G**
| hartrees |
Energy at 0K | -207.959285 |
Energy at 298.15K | -207.962645 |
HF Energy | -207.959285 |
Nuclear repulsion energy | 101.905734 |
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 B3LYP/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 |
3812 |
3662 |
31.16 |
68.82 |
0.28 |
0.43 |
2 |
A |
3107 |
2986 |
5.74 |
83.82 |
0.40 |
0.57 |
3 |
A |
3017 |
2898 |
28.29 |
109.67 |
0.17 |
0.29 |
4 |
A |
2366 |
2273 |
0.16 |
52.48 |
0.27 |
0.42 |
5 |
A |
1496 |
1437 |
2.47 |
15.92 |
0.66 |
0.80 |
6 |
A |
1417 |
1361 |
47.04 |
8.56 |
0.73 |
0.85 |
7 |
A |
1380 |
1326 |
2.18 |
7.49 |
0.73 |
0.84 |
8 |
A |
1224 |
1176 |
18.98 |
4.90 |
0.61 |
0.76 |
9 |
A |
1084 |
1041 |
98.29 |
5.93 |
0.30 |
0.46 |
10 |
A |
990 |
952 |
26.22 |
0.60 |
0.50 |
0.67 |
11 |
A |
897 |
862 |
16.82 |
1.98 |
0.17 |
0.29 |
12 |
A |
582 |
559 |
2.08 |
1.72 |
0.31 |
0.47 |
13 |
A |
397 |
381 |
61.98 |
1.30 |
0.72 |
0.84 |
14 |
A |
311 |
299 |
92.42 |
5.37 |
0.75 |
0.86 |
15 |
A |
214 |
206 |
8.61 |
4.59 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11147.1 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 10710.1 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 B3LYP/6-31G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.573 |
0.590 |
0.038 |
C2 |
0.827 |
0.119 |
-0.007 |
O3 |
-1.510 |
-0.456 |
-0.112 |
H4 |
-0.712 |
1.159 |
0.970 |
H5 |
-0.737 |
1.281 |
-0.794 |
H6 |
-1.406 |
-1.066 |
0.631 |
N7 |
1.916 |
-0.283 |
-0.014 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4781 | 1.4119 | 1.1001 | 1.0939 | 1.9460 | 2.6381 |
C2 | 1.4781 | | 2.4089 | 2.0984 | 2.1017 | 2.6074 | 1.1605 | O3 | 1.4119 | 2.4089 | | 2.1004 | 2.0197 | 0.9669 | 3.4311 | H4 | 1.1001 | 2.0984 | 2.1004 | | 1.7679 | 2.3543 | 3.1549 | H5 | 1.0939 | 2.1017 | 2.0197 | 1.7679 | | 2.8260 | 3.1768 | H6 | 1.9460 | 2.6074 | 0.9669 | 2.3543 | 2.8260 | | 3.4733 | N7 | 2.6381 | 1.1605 | 3.4311 | 3.1549 | 3.1768 | 3.4733 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
177.826 |
|
C1 |
O3 |
H6 |
108.331 |
C2 |
C1 |
O3 |
112.910 |
|
C2 |
C1 |
H4 |
108.062 |
C2 |
C1 |
H5 |
108.678 |
|
O3 |
C1 |
H4 |
112.883 |
O3 |
C1 |
H5 |
106.727 |
|
H4 |
C1 |
H5 |
107.366 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.013 |
|
|
|
2 |
C |
0.318 |
|
|
|
3 |
O |
-0.508 |
|
|
|
4 |
H |
0.142 |
|
|
|
5 |
H |
0.167 |
|
|
|
6 |
H |
0.322 |
|
|
|
7 |
N |
-0.455 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.384 |
1.115 |
1.351 |
2.958 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.296 |
1.238 |
-1.959 |
y |
1.238 |
-20.351 |
-1.759 |
z |
-1.959 |
-1.759 |
-21.497 |
|
Traceless |
| x | y | z |
x |
-10.372 |
1.238 |
-1.959 |
y |
1.238 |
6.045 |
-1.759 |
z |
-1.959 |
-1.759 |
4.326 |
|
Polar |
3z2-r2 | 8.652 |
x2-y2 | -10.945 |
xy | 1.238 |
xz | -1.959 |
yz | -1.759 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.325 |
-0.461 |
-0.042 |
y |
-0.461 |
3.537 |
-0.150 |
z |
-0.042 |
-0.150 |
3.015 |
<r2> (average value of r
2) Å
2
<r2> |
78.852 |
(<r2>)1/2 |
8.880 |