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S1C2
Vibrational Frequencies calculated at B97D3/cc-pVTZ
Geometric Data calculated at B97D3/cc-pVTZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B97D3/cc-pVTZ
| hartrees |
Energy at 0K | -207.909345 |
Energy at 298.15K | -207.912615 |
HF Energy | -207.909345 |
Nuclear repulsion energy | 101.873587 |
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 B97D3/cc-pVTZ
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 |
3734 |
3682 |
33.21 |
65.32 |
0.23 |
0.37 |
2 |
A |
3039 |
2997 |
5.38 |
88.31 |
0.34 |
0.51 |
3 |
A |
2949 |
2908 |
29.71 |
126.82 |
0.14 |
0.25 |
4 |
A |
2273 |
2241 |
0.16 |
74.99 |
0.20 |
0.34 |
5 |
A |
1453 |
1433 |
3.57 |
10.73 |
0.58 |
0.73 |
6 |
A |
1387 |
1368 |
40.54 |
4.74 |
0.75 |
0.86 |
7 |
A |
1338 |
1319 |
1.78 |
4.14 |
0.72 |
0.83 |
8 |
A |
1201 |
1185 |
15.93 |
3.21 |
0.46 |
0.63 |
9 |
A |
1023 |
1009 |
87.18 |
6.13 |
0.31 |
0.47 |
10 |
A |
966 |
953 |
30.68 |
0.54 |
0.49 |
0.66 |
11 |
A |
875 |
863 |
12.52 |
2.00 |
0.09 |
0.17 |
12 |
A |
569 |
561 |
1.61 |
2.03 |
0.18 |
0.30 |
13 |
A |
367 |
362 |
37.18 |
0.91 |
0.73 |
0.84 |
14 |
A |
286 |
282 |
91.50 |
2.81 |
0.75 |
0.86 |
15 |
A |
205 |
202 |
9.60 |
3.20 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 10833.4 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 10681.7 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 B97D3/cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.568 |
0.594 |
0.038 |
C2 |
0.826 |
0.122 |
-0.007 |
O3 |
-1.514 |
-0.456 |
-0.107 |
H4 |
-0.709 |
1.161 |
0.971 |
H5 |
-0.737 |
1.283 |
-0.796 |
H6 |
-1.368 |
-1.093 |
0.604 |
N7 |
1.912 |
-0.286 |
-0.015 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4729 | 1.4206 | 1.1008 | 1.0944 | 1.9508 | 2.6321 |
C2 | 1.4729 | | 2.4120 | 2.0961 | 2.1001 | 2.5807 | 1.1597 | O3 | 1.4206 | 2.4120 | | 2.1043 | 2.0250 | 0.9663 | 3.4310 | H4 | 1.1008 | 2.0961 | 2.1043 | | 1.7716 | 2.3772 | 3.1515 | H5 | 1.0944 | 2.1001 | 2.0250 | 1.7716 | | 2.8288 | 3.1751 | H6 | 1.9508 | 2.5807 | 0.9663 | 2.3772 | 2.8288 | | 3.4334 | N7 | 2.6321 | 1.1597 | 3.4310 | 3.1515 | 3.1751 | 3.4334 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
177.699 |
|
C1 |
O3 |
H6 |
108.121 |
C2 |
C1 |
O3 |
112.925 |
|
C2 |
C1 |
H4 |
108.191 |
C2 |
C1 |
H5 |
108.878 |
|
O3 |
C1 |
H4 |
112.521 |
O3 |
C1 |
H5 |
106.532 |
|
H4 |
C1 |
H5 |
107.609 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.059 |
|
|
|
2 |
C |
-0.126 |
|
|
|
3 |
O |
-0.298 |
|
|
|
4 |
H |
0.082 |
|
|
|
5 |
H |
0.108 |
|
|
|
6 |
H |
0.208 |
|
|
|
7 |
N |
-0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.419 |
1.100 |
1.192 |
2.913 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.590 |
1.189 |
-1.681 |
y |
1.189 |
-20.579 |
-1.683 |
z |
-1.681 |
-1.683 |
-21.860 |
|
Traceless |
| x | y | z |
x |
-10.370 |
1.189 |
-1.681 |
y |
1.189 |
6.146 |
-1.683 |
z |
-1.681 |
-1.683 |
4.224 |
|
Polar |
3z2-r2 | 8.448 |
x2-y2 | -11.011 |
xy | 1.189 |
xz | -1.681 |
yz | -1.683 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.194 |
-0.436 |
-0.033 |
y |
-0.436 |
4.256 |
-0.096 |
z |
-0.033 |
-0.096 |
3.664 |
<r2> (average value of r
2) Å
2
<r2> |
78.948 |
(<r2>)1/2 |
8.885 |