Jump to
S1C2
S1C3
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -168.937931 |
| Energy at 298.15K | -168.941992 |
| HF Energy | -168.937931 |
| Nuclear repulsion energy | 71.812113 |
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/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' |
4197 |
3796 |
83.67 |
|
|
|
| 2 |
A' |
3791 |
3429 |
3.73 |
|
|
|
| 3 |
A' |
3240 |
2930 |
70.93 |
|
|
|
| 4 |
A' |
1937 |
1752 |
261.23 |
|
|
|
| 5 |
A' |
1588 |
1436 |
27.54 |
|
|
|
| 6 |
A' |
1467 |
1327 |
224.61 |
|
|
|
| 7 |
A' |
1309 |
1184 |
91.79 |
|
|
|
| 8 |
A' |
1157 |
1047 |
193.93 |
|
|
|
| 9 |
A' |
670 |
606 |
0.51 |
|
|
|
| 10 |
A" |
1183 |
1070 |
12.95 |
|
|
|
| 11 |
A" |
916 |
828 |
62.52 |
|
|
|
| 12 |
A" |
367 |
332 |
106.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10910.9 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 9867.9 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.363 |
0.000 |
| O2 |
-0.991 |
-0.533 |
0.000 |
| N3 |
1.186 |
0.002 |
0.000 |
| H4 |
-0.336 |
1.394 |
0.000 |
| H5 |
-1.831 |
-0.114 |
0.000 |
| H6 |
1.795 |
0.794 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3357 | 1.2395 | 1.0853 | 1.8920 | 1.8464 |
O2 | 1.3357 | | 2.2416 | 2.0354 | 0.9386 | 3.0860 | N3 | 1.2395 | 2.2416 | | 2.0632 | 3.0191 | 0.9993 | H4 | 1.0853 | 2.0354 | 2.0632 | | 2.1235 | 2.2148 | H5 | 1.8920 | 0.9386 | 3.0191 | 2.1235 | | 3.7382 | H6 | 1.8464 | 3.0860 | 0.9993 | 2.2148 | 3.7382 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
111.400 |
|
C1 |
N3 |
H6 |
110.661 |
| O2 |
C1 |
N3 |
120.980 |
|
O2 |
C1 |
H4 |
114.037 |
| N3 |
C1 |
H4 |
124.984 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.228 |
|
|
|
| 2 |
O |
-0.563 |
|
|
|
| 3 |
N |
-0.566 |
|
|
|
| 4 |
H |
0.174 |
|
|
|
| 5 |
H |
0.429 |
|
|
|
| 6 |
H |
0.298 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.281 |
3.671 |
0.000 |
4.322 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.892 |
1.224 |
0.000 |
| y |
1.224 |
-17.862 |
0.000 |
| z |
0.000 |
0.000 |
-18.727 |
|
| Traceless |
| | x | y | z |
| x |
4.402 |
1.224 |
0.000 |
| y |
1.224 |
-1.553 |
0.000 |
| z |
0.000 |
0.000 |
-2.850 |
|
| Polar |
| 3z2-r2 | -5.700 |
| x2-y2 | 3.970 |
| xy | 1.224 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.478 |
-0.066 |
0.000 |
| y |
-0.066 |
2.610 |
0.000 |
| z |
0.000 |
0.000 |
1.638 |
<r2> (average value of r
2) Å
2
| <r2> |
40.548 |
| (<r2>)1/2 |
6.368 |
Jump to
S1C1
S1C3
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -168.949734 |
| Energy at 298.15K | -168.954004 |
| HF Energy | -168.949734 |
| Nuclear repulsion energy | 72.176718 |
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/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' |
4116 |
3723 |
70.16 |
|
|
|
| 2 |
A' |
3798 |
3435 |
5.17 |
|
|
|
| 3 |
A' |
3317 |
3000 |
42.01 |
|
|
|
| 4 |
A' |
1907 |
1724 |
374.41 |
|
|
|
| 5 |
A' |
1554 |
1405 |
43.89 |
|
|
|
| 6 |
A' |
1490 |
1348 |
2.73 |
|
|
|
| 7 |
A' |
1324 |
1197 |
130.32 |
|
|
|
| 8 |
A' |
1171 |
1059 |
210.59 |
|
|
|
| 9 |
A' |
640 |
579 |
59.77 |
|
|
|
| 10 |
A" |
1192 |
1078 |
1.98 |
|
|
|
| 11 |
A" |
918 |
830 |
33.36 |
|
|
|
| 12 |
A" |
662 |
599 |
254.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 11043.9 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 9988.1 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 HF/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.408 |
0.000 |
| O2 |
-1.095 |
-0.341 |
0.000 |
| N3 |
1.144 |
-0.080 |
0.000 |
| H4 |
-0.257 |
1.457 |
0.000 |
| H5 |
-0.842 |
-1.251 |
0.000 |
| H6 |
1.849 |
0.628 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3266 | 1.2439 | 1.0801 | 1.8600 | 1.8619 |
O2 | 1.3266 | | 2.2546 | 1.9838 | 0.9443 | 3.0993 | N3 | 1.2439 | 2.2546 | | 2.0794 | 2.3058 | 0.9988 | H4 | 1.0801 | 1.9838 | 2.0794 | | 2.7702 | 2.2626 | H5 | 1.8600 | 0.9443 | 2.3058 | 2.7702 | | 3.2819 | H6 | 1.8619 | 3.0993 | 0.9988 | 2.2626 | 3.2819 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
108.812 |
|
C1 |
N3 |
H6 |
111.779 |
| O2 |
C1 |
N3 |
122.564 |
|
O2 |
C1 |
H4 |
110.618 |
| N3 |
C1 |
H4 |
126.817 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.265 |
|
|
|
| 2 |
O |
-0.591 |
|
|
|
| 3 |
N |
-0.630 |
|
|
|
| 4 |
H |
0.211 |
|
|
|
| 5 |
H |
0.437 |
|
|
|
| 6 |
H |
0.308 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.083 |
1.194 |
0.000 |
1.197 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.993 |
3.545 |
0.000 |
| y |
3.545 |
-13.651 |
0.000 |
| z |
0.000 |
0.000 |
-18.717 |
|
| Traceless |
| | x | y | z |
| x |
-3.809 |
3.545 |
0.000 |
| y |
3.545 |
5.704 |
0.000 |
| z |
0.000 |
0.000 |
-1.895 |
|
| Polar |
| 3z2-r2 | -3.790 |
| x2-y2 | -6.342 |
| xy | 3.545 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.998 |
-0.052 |
0.000 |
| y |
-0.052 |
2.955 |
0.000 |
| z |
0.000 |
0.000 |
1.624 |
<r2> (average value of r
2) Å
2
| <r2> |
39.909 |
| (<r2>)1/2 |
6.317 |
Jump to
S1C1
S1C2
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -168.943288 |
| Energy at 298.15K | -168.947486 |
| HF Energy | -168.943288 |
| Nuclear repulsion energy | 71.846674 |
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/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' |
4142 |
3746 |
45.14 |
|
|
|
| 2 |
A' |
3716 |
3360 |
5.26 |
|
|
|
| 3 |
A' |
3375 |
3052 |
22.13 |
|
|
|
| 4 |
A' |
1902 |
1720 |
382.33 |
|
|
|
| 5 |
A' |
1537 |
1390 |
2.54 |
|
|
|
| 6 |
A' |
1481 |
1340 |
30.24 |
|
|
|
| 7 |
A' |
1247 |
1127 |
326.90 |
|
|
|
| 8 |
A' |
1188 |
1074 |
37.14 |
|
|
|
| 9 |
A' |
649 |
587 |
46.24 |
|
|
|
| 10 |
A" |
1200 |
1086 |
63.69 |
|
|
|
| 11 |
A" |
952 |
861 |
102.45 |
|
|
|
| 12 |
A" |
527 |
477 |
113.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10957.5 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 9910.0 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.437 |
0.000 |
| O2 |
-1.079 |
-0.352 |
0.000 |
| N3 |
1.203 |
0.122 |
0.000 |
| H4 |
-0.297 |
1.471 |
0.000 |
| H5 |
-0.848 |
-1.265 |
0.000 |
| H6 |
1.359 |
-0.870 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3368 | 1.2436 | 1.0757 | 1.9015 | 1.8856 |
O2 | 1.3368 | | 2.3310 | 1.9835 | 0.9422 | 2.4926 | N3 | 1.2436 | 2.3310 | | 2.0174 | 2.4757 | 1.0045 | H4 | 1.0757 | 1.9835 | 2.0174 | | 2.7908 | 2.8677 | H5 | 1.9015 | 0.9422 | 2.4757 | 2.7908 | | 2.2415 | H6 | 1.8856 | 2.4926 | 1.0045 | 2.8677 | 2.2415 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
111.930 |
|
C1 |
N3 |
H6 |
113.595 |
| O2 |
C1 |
N3 |
129.162 |
|
O2 |
C1 |
H4 |
110.131 |
| N3 |
C1 |
H4 |
120.707 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.270 |
|
|
|
| 2 |
O |
-0.596 |
|
|
|
| 3 |
N |
-0.611 |
|
|
|
| 4 |
H |
0.241 |
|
|
|
| 5 |
H |
0.420 |
|
|
|
| 6 |
H |
0.277 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.046 |
-2.000 |
0.000 |
2.257 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.695 |
-2.101 |
0.000 |
| y |
-2.101 |
-12.612 |
0.000 |
| z |
0.000 |
0.000 |
-18.690 |
|
| Traceless |
| | x | y | z |
| x |
-8.044 |
-2.101 |
0.000 |
| y |
-2.101 |
8.580 |
0.000 |
| z |
0.000 |
0.000 |
-0.536 |
|
| Polar |
| 3z2-r2 | -1.073 |
| x2-y2 | -11.082 |
| xy | -2.101 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.820 |
-0.289 |
0.000 |
| y |
-0.289 |
3.125 |
0.000 |
| z |
0.000 |
0.000 |
1.643 |
<r2> (average value of r
2) Å
2
| <r2> |
40.315 |
| (<r2>)1/2 |
6.349 |