Jump to
S1C2
S1C3
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -168.977965 |
Energy at 298.15K | -168.981940 |
HF Energy | -168.977965 |
Nuclear repulsion energy | 70.804441 |
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 LSDA/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' |
3696 |
3627 |
53.27 |
|
|
|
2 |
A' |
3459 |
3394 |
5.23 |
|
|
|
3 |
A' |
2934 |
2879 |
79.37 |
|
|
|
4 |
A' |
1783 |
1750 |
187.51 |
|
|
|
5 |
A' |
1401 |
1375 |
16.51 |
|
|
|
6 |
A' |
1314 |
1289 |
165.86 |
|
|
|
7 |
A' |
1178 |
1156 |
37.16 |
|
|
|
8 |
A' |
1045 |
1025 |
226.36 |
|
|
|
9 |
A' |
613 |
601 |
2.48 |
|
|
|
10 |
A" |
999 |
980 |
4.86 |
|
|
|
11 |
A" |
809 |
794 |
76.35 |
|
|
|
12 |
A" |
419 |
411 |
66.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9824.3 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 9640.6 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.373 |
0.000 |
O2 |
-1.002 |
-0.522 |
0.000 |
N3 |
1.196 |
-0.031 |
0.000 |
H4 |
-0.341 |
1.432 |
0.000 |
H5 |
-1.854 |
-0.043 |
0.000 |
H6 |
1.840 |
0.769 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3438 | 1.2625 | 1.1128 | 1.8996 | 1.8821 |
O2 | 1.3438 | | 2.2527 | 2.0630 | 0.9769 | 3.1218 | N3 | 1.2625 | 2.2527 | | 2.1222 | 3.0498 | 1.0269 | H4 | 1.1128 | 2.0630 | 2.1222 | | 2.1124 | 2.2796 | H5 | 1.8996 | 0.9769 | 3.0498 | 2.1124 | | 3.7817 | H6 | 1.8821 | 3.1218 | 1.0269 | 2.2796 | 3.7817 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
108.853 |
|
C1 |
N3 |
H6 |
110.168 |
O2 |
C1 |
N3 |
119.587 |
|
O2 |
C1 |
H4 |
113.905 |
N3 |
C1 |
H4 |
126.509 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.144 |
|
|
|
2 |
O |
-0.485 |
|
|
|
3 |
N |
-0.518 |
|
|
|
4 |
H |
0.130 |
|
|
|
5 |
H |
0.420 |
|
|
|
6 |
H |
0.309 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.084 |
3.090 |
0.000 |
3.727 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-13.233 |
1.318 |
0.000 |
y |
1.318 |
-17.828 |
0.000 |
z |
0.000 |
0.000 |
-18.597 |
|
Traceless |
| x | y | z |
x |
4.980 |
1.318 |
0.000 |
y |
1.318 |
-1.913 |
0.000 |
z |
0.000 |
0.000 |
-3.067 |
|
Polar |
3z2-r2 | -6.133 |
x2-y2 | 4.595 |
xy | 1.318 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.986 |
0.008 |
0.000 |
y |
0.008 |
2.973 |
0.000 |
z |
0.000 |
0.000 |
1.475 |
<r2> (average value of r
2) Å
2
<r2> |
40.996 |
(<r2>)1/2 |
6.403 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -168.989270 |
Energy at 298.15K | -168.993401 |
HF Energy | -168.989270 |
Nuclear repulsion energy | 71.201339 |
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 LSDA/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' |
3542 |
3476 |
29.75 |
|
|
|
2 |
A' |
3456 |
3392 |
4.58 |
|
|
|
3 |
A' |
3043 |
2986 |
36.51 |
|
|
|
4 |
A' |
1749 |
1716 |
235.67 |
|
|
|
5 |
A' |
1376 |
1350 |
25.86 |
|
|
|
6 |
A' |
1349 |
1324 |
0.61 |
|
|
|
7 |
A' |
1176 |
1154 |
142.69 |
|
|
|
8 |
A' |
1059 |
1039 |
126.85 |
|
|
|
9 |
A' |
571 |
561 |
58.41 |
|
|
|
10 |
A" |
1008 |
989 |
0.98 |
|
|
|
11 |
A" |
812 |
797 |
14.97 |
|
|
|
12 |
A" |
672 |
659 |
209.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9906.3 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 9721.1 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.419 |
0.000 |
O2 |
-1.111 |
-0.318 |
0.000 |
N3 |
1.149 |
-0.115 |
0.000 |
H4 |
-0.259 |
1.494 |
0.000 |
H5 |
-0.790 |
-1.253 |
0.000 |
H6 |
1.893 |
0.593 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3339 | 1.2676 | 1.1052 | 1.8495 | 1.9012 |
O2 | 1.3339 | | 2.2699 | 2.0027 | 0.9883 | 3.1399 | N3 | 1.2676 | 2.2699 | | 2.1381 | 2.2487 | 1.0270 | H4 | 1.1052 | 2.0027 | 2.1381 | | 2.7977 | 2.3329 | H5 | 1.8495 | 0.9883 | 2.2487 | 2.7977 | | 3.2571 | H6 | 1.9012 | 3.1399 | 1.0270 | 2.3329 | 3.2571 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
104.602 |
|
C1 |
N3 |
H6 |
111.475 |
O2 |
C1 |
N3 |
121.496 |
|
O2 |
C1 |
H4 |
110.029 |
N3 |
C1 |
H4 |
128.475 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.170 |
|
|
|
2 |
O |
-0.496 |
|
|
|
3 |
N |
-0.566 |
|
|
|
4 |
H |
0.165 |
|
|
|
5 |
H |
0.414 |
|
|
|
6 |
H |
0.313 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.135 |
0.872 |
0.000 |
0.882 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.850 |
3.337 |
0.000 |
y |
3.337 |
-14.116 |
0.000 |
z |
0.000 |
0.000 |
-18.597 |
|
Traceless |
| x | y | z |
x |
-2.493 |
3.337 |
0.000 |
y |
3.337 |
4.607 |
0.000 |
z |
0.000 |
0.000 |
-2.114 |
|
Polar |
3z2-r2 | -4.228 |
x2-y2 | -4.734 |
xy | 3.337 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.389 |
0.147 |
0.000 |
y |
0.147 |
3.440 |
0.000 |
z |
0.000 |
0.000 |
1.471 |
<r2> (average value of r
2) Å
2
<r2> |
40.252 |
(<r2>)1/2 |
6.344 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -168.982976 |
Energy at 298.15K | -168.987048 |
HF Energy | -168.982976 |
Nuclear repulsion energy | 70.682967 |
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 LSDA/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' |
3596 |
3529 |
13.83 |
|
|
|
2 |
A' |
3347 |
3285 |
7.75 |
|
|
|
3 |
A' |
3109 |
3051 |
10.42 |
|
|
|
4 |
A' |
1751 |
1718 |
247.00 |
|
|
|
5 |
A' |
1364 |
1339 |
0.19 |
|
|
|
6 |
A' |
1324 |
1300 |
22.03 |
|
|
|
7 |
A' |
1118 |
1097 |
169.03 |
|
|
|
8 |
A' |
1054 |
1035 |
136.31 |
|
|
|
9 |
A' |
577 |
566 |
37.44 |
|
|
|
10 |
A" |
1030 |
1011 |
73.13 |
|
|
|
11 |
A" |
824 |
809 |
55.27 |
|
|
|
12 |
A" |
565 |
554 |
75.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9830.0 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 9646.1 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.433 |
0.000 |
O2 |
-1.104 |
-0.339 |
0.000 |
N3 |
1.226 |
0.115 |
0.000 |
H4 |
-0.296 |
1.493 |
0.000 |
H5 |
-0.824 |
-1.282 |
0.000 |
H6 |
1.370 |
-0.909 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
C1 | | 1.3466 | 1.2660 | 1.1006 | 1.9025 | 1.9185 |
O2 | 1.3466 | | 2.3729 | 2.0018 | 0.9838 | 2.5391 | N3 | 1.2660 | 2.3729 | | 2.0526 | 2.4803 | 1.0351 | H4 | 1.1006 | 2.0018 | 2.0526 | | 2.8246 | 2.9240 | H5 | 1.9025 | 0.9838 | 2.4803 | 2.8246 | | 2.2257 | H6 | 1.9185 | 2.5391 | 1.0351 | 2.9240 | 2.2257 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
O2 |
H5 |
108.444 |
|
C1 |
N3 |
H6 |
112.584 |
O2 |
C1 |
N3 |
130.506 |
|
O2 |
C1 |
H4 |
109.357 |
N3 |
C1 |
H4 |
120.137 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.127 |
|
|
|
2 |
O |
-0.488 |
|
|
|
3 |
N |
-0.511 |
|
|
|
4 |
H |
0.191 |
|
|
|
5 |
H |
0.401 |
|
|
|
6 |
H |
0.281 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.005 |
-2.044 |
0.000 |
2.278 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.511 |
-1.752 |
0.000 |
y |
-1.752 |
-12.894 |
0.000 |
z |
0.000 |
0.000 |
-18.606 |
|
Traceless |
| x | y | z |
x |
-6.761 |
-1.752 |
0.000 |
y |
-1.752 |
7.665 |
0.000 |
z |
0.000 |
0.000 |
-0.904 |
|
Polar |
3z2-r2 | -1.807 |
x2-y2 | -9.617 |
xy | -1.752 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.140 |
-0.147 |
0.000 |
y |
-0.147 |
3.675 |
0.000 |
z |
0.000 |
0.000 |
1.492 |
<r2> (average value of r
2) Å
2
<r2> |
40.981 |
(<r2>)1/2 |
6.402 |