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S1C2
Vibrational Frequencies calculated at B1B95/6-311G**
Geometric Data calculated at B1B95/6-311G**
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B1B95/6-311G**
| hartrees |
Energy at 0K | -207.929543 |
Energy at 298.15K | -207.932938 |
HF Energy | -207.929543 |
Nuclear repulsion energy | 102.716373 |
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 B1B95/6-311G**
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 |
3887 |
3732 |
49.00 |
58.32 |
0.28 |
0.44 |
2 |
A |
3131 |
3006 |
3.93 |
81.96 |
0.39 |
0.56 |
3 |
A |
3042 |
2920 |
25.19 |
117.13 |
0.15 |
0.25 |
4 |
A |
2391 |
2296 |
0.43 |
58.32 |
0.24 |
0.38 |
5 |
A |
1487 |
1428 |
4.66 |
11.43 |
0.68 |
0.81 |
6 |
A |
1421 |
1364 |
43.33 |
6.08 |
0.72 |
0.84 |
7 |
A |
1379 |
1324 |
1.23 |
4.97 |
0.75 |
0.86 |
8 |
A |
1230 |
1181 |
16.85 |
3.41 |
0.60 |
0.75 |
9 |
A |
1114 |
1070 |
107.96 |
5.37 |
0.32 |
0.49 |
10 |
A |
991 |
951 |
19.65 |
0.57 |
0.44 |
0.61 |
11 |
A |
912 |
876 |
16.38 |
1.98 |
0.13 |
0.23 |
12 |
A |
593 |
569 |
2.21 |
1.92 |
0.27 |
0.43 |
13 |
A |
398 |
382 |
57.03 |
1.18 |
0.73 |
0.84 |
14 |
A |
313 |
300 |
97.83 |
4.26 |
0.75 |
0.85 |
15 |
A |
217 |
208 |
9.54 |
4.23 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 11251.5 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 10802.6 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 B1B95/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.568 |
0.585 |
0.038 |
C2 |
0.821 |
0.115 |
-0.006 |
O3 |
-1.500 |
-0.450 |
-0.110 |
H4 |
-0.703 |
1.150 |
0.966 |
H5 |
-0.725 |
1.274 |
-0.791 |
H6 |
-1.389 |
-1.065 |
0.617 |
N7 |
1.900 |
-0.280 |
-0.015 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
H5 |
H6 |
N7 |
C1 | | 1.4670 | 1.4005 | 1.0954 | 1.0892 | 1.9316 | 2.6160 |
C2 | 1.4670 | | 2.3912 | 2.0834 | 2.0853 | 2.5816 | 1.1494 | O3 | 1.4005 | 2.3912 | | 2.0866 | 2.0093 | 0.9585 | 3.4060 | H4 | 1.0954 | 2.0834 | 2.0866 | | 1.7615 | 2.3451 | 3.1283 | H5 | 1.0892 | 2.0853 | 2.0093 | 1.7615 | | 2.8096 | 3.1480 | H6 | 1.9316 | 2.5816 | 0.9585 | 2.3451 | 2.8096 | | 3.4400 | N7 | 2.6160 | 1.1494 | 3.4060 | 3.1283 | 3.1480 | 3.4400 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N7 |
178.057 |
|
C1 |
O3 |
H6 |
108.476 |
C2 |
C1 |
O3 |
112.981 |
|
C2 |
C1 |
H4 |
107.914 |
C2 |
C1 |
H5 |
108.427 |
|
O3 |
C1 |
H4 |
112.872 |
O3 |
C1 |
H5 |
106.949 |
|
H4 |
C1 |
H5 |
107.480 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.012 |
|
|
|
2 |
C |
0.033 |
|
|
|
3 |
O |
-0.371 |
|
|
|
4 |
H |
0.157 |
|
|
|
5 |
H |
0.169 |
|
|
|
6 |
H |
0.255 |
|
|
|
7 |
N |
-0.255 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.391 |
1.142 |
1.343 |
2.970 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.561 |
1.185 |
-1.938 |
y |
1.185 |
-20.415 |
-1.751 |
z |
-1.938 |
-1.751 |
-21.609 |
|
Traceless |
| x | y | z |
x |
-10.549 |
1.185 |
-1.938 |
y |
1.185 |
6.170 |
-1.751 |
z |
-1.938 |
-1.751 |
4.379 |
|
Polar |
3z2-r2 | 8.758 |
x2-y2 | -11.146 |
xy | 1.185 |
xz | -1.938 |
yz | -1.751 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.455 |
-0.461 |
-0.041 |
y |
-0.461 |
3.680 |
-0.122 |
z |
-0.041 |
-0.122 |
3.144 |
<r2> (average value of r
2) Å
2
<r2> |
77.958 |
(<r2>)1/2 |
8.829 |