Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -169.723145 |
| Energy at 298.15K | -169.727158 |
| HF Energy | -169.723145 |
| Nuclear repulsion energy | 71.053025 |
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 HSEh1PBE/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' |
3868 |
3712 |
50.27 |
|
|
|
| 2 |
A' |
3566 |
3422 |
2.85 |
|
|
|
| 3 |
A' |
3036 |
2913 |
82.80 |
|
|
|
| 4 |
A' |
1800 |
1727 |
201.56 |
|
|
|
| 5 |
A' |
1455 |
1397 |
15.68 |
|
|
|
| 6 |
A' |
1359 |
1304 |
181.32 |
|
|
|
| 7 |
A' |
1216 |
1166 |
59.51 |
|
|
|
| 8 |
A' |
1081 |
1037 |
215.45 |
|
|
|
| 9 |
A' |
628 |
602 |
1.11 |
|
|
|
| 10 |
A" |
1053 |
1011 |
6.82 |
|
|
|
| 11 |
A" |
842 |
808 |
72.77 |
|
|
|
| 12 |
A" |
403 |
387 |
82.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10152.8 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 9742.6 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.371 |
0.000 |
| O2 |
-0.999 |
-0.532 |
0.000 |
| N3 |
1.195 |
-0.013 |
0.000 |
| H4 |
-0.344 |
1.416 |
0.000 |
| H5 |
-1.845 |
-0.079 |
0.000 |
| H6 |
1.818 |
0.788 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3473 | 1.2553 | 1.0995 | 1.8991 | 1.8649 |
O2 | 1.3473 | | 2.2550 | 2.0553 | 0.9594 | 3.1112 | N3 | 1.2553 | 2.2550 | | 2.0998 | 3.0407 | 1.0147 | H4 | 1.0995 | 2.0553 | 2.0998 | | 2.1185 | 2.2507 | H5 | 1.8991 | 0.9594 | 3.0407 | 2.1185 | | 3.7640 | H6 | 1.8649 | 3.1112 | 1.0147 | 2.2507 | 3.7640 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
109.696 |
|
C1 |
N3 |
H6 |
110.026 |
| O2 |
C1 |
N3 |
120.054 |
|
O2 |
C1 |
H4 |
113.900 |
| N3 |
C1 |
H4 |
126.046 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.099 |
|
|
|
| 2 |
O |
-0.462 |
|
|
|
| 3 |
N |
-0.497 |
|
|
|
| 4 |
H |
0.169 |
|
|
|
| 5 |
H |
0.403 |
|
|
|
| 6 |
H |
0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.151 |
3.347 |
0.000 |
3.979 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.594 |
1.279 |
0.000 |
| y |
1.279 |
-17.872 |
0.000 |
| z |
0.000 |
0.000 |
-18.760 |
|
| Traceless |
| | x | y | z |
| x |
4.722 |
1.279 |
0.000 |
| y |
1.279 |
-1.695 |
0.000 |
| z |
0.000 |
0.000 |
-3.027 |
|
| Polar |
| 3z2-r2 | -6.053 |
| x2-y2 | 4.278 |
| xy | 1.279 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.833 |
-0.019 |
0.000 |
| y |
-0.019 |
2.922 |
0.000 |
| z |
0.000 |
0.000 |
1.719 |
<r2> (average value of r
2) Å
2
| <r2> |
40.996 |
| (<r2>)1/2 |
6.403 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -169.734327 |
| Energy at 298.15K | -169.738513 |
| HF Energy | -169.734327 |
| Nuclear repulsion energy | 71.438698 |
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 HSEh1PBE/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' |
3757 |
3605 |
31.63 |
|
|
|
| 2 |
A' |
3569 |
3424 |
2.71 |
|
|
|
| 3 |
A' |
3128 |
3002 |
43.07 |
|
|
|
| 4 |
A' |
1770 |
1699 |
281.31 |
|
|
|
| 5 |
A' |
1422 |
1365 |
27.22 |
|
|
|
| 6 |
A' |
1395 |
1339 |
1.69 |
|
|
|
| 7 |
A' |
1223 |
1174 |
122.60 |
|
|
|
| 8 |
A' |
1091 |
1047 |
174.76 |
|
|
|
| 9 |
A' |
594 |
570 |
55.98 |
|
|
|
| 10 |
A" |
1063 |
1020 |
0.17 |
|
|
|
| 11 |
A" |
843 |
809 |
27.14 |
|
|
|
| 12 |
A" |
668 |
641 |
220.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10261.9 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 9847.3 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.415 |
0.000 |
| O2 |
-1.107 |
-0.334 |
0.000 |
| N3 |
1.152 |
-0.094 |
0.000 |
| H4 |
-0.267 |
1.475 |
0.000 |
| H5 |
-0.817 |
-1.257 |
0.000 |
| H6 |
1.872 |
0.621 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3367 | 1.2598 | 1.0931 | 1.8615 | 1.8833 |
O2 | 1.3367 | | 2.2719 | 1.9947 | 0.9672 | 3.1282 | N3 | 1.2598 | 2.2719 | | 2.1160 | 2.2875 | 1.0144 | H4 | 1.0931 | 1.9947 | 2.1160 | | 2.7872 | 2.3035 | H5 | 1.8615 | 0.9672 | 2.2875 | 2.7872 | | 3.2803 | H6 | 1.8833 | 3.1282 | 1.0144 | 2.3035 | 3.2803 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
106.696 |
|
C1 |
N3 |
H6 |
111.351 |
| O2 |
C1 |
N3 |
122.051 |
|
O2 |
C1 |
H4 |
109.955 |
| N3 |
C1 |
H4 |
127.994 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.129 |
|
|
|
| 2 |
O |
-0.484 |
|
|
|
| 3 |
N |
-0.553 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
0.402 |
|
|
|
| 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 |
| |
0.136 |
0.993 |
0.000 |
1.003 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.481 |
3.466 |
0.000 |
| y |
3.466 |
-13.900 |
0.000 |
| z |
0.000 |
0.000 |
-18.752 |
|
| Traceless |
| | x | y | z |
| x |
-3.155 |
3.466 |
0.000 |
| y |
3.466 |
5.216 |
0.000 |
| z |
0.000 |
0.000 |
-2.061 |
|
| Polar |
| 3z2-r2 | -4.122 |
| x2-y2 | -5.581 |
| xy | 3.466 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.327 |
0.065 |
0.000 |
| y |
0.065 |
3.327 |
0.000 |
| z |
0.000 |
0.000 |
1.704 |
<r2> (average value of r
2) Å
2
| <r2> |
40.325 |
| (<r2>)1/2 |
6.350 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-311G*
| | hartrees |
| Energy at 0K | -169.728227 |
| Energy at 298.15K | -169.732346 |
| HF Energy | -169.728227 |
| Nuclear repulsion energy | 70.972064 |
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 HSEh1PBE/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' |
3791 |
3638 |
18.04 |
|
|
|
| 2 |
A' |
3472 |
3331 |
9.35 |
|
|
|
| 3 |
A' |
3193 |
3064 |
16.34 |
|
|
|
| 4 |
A' |
1767 |
1696 |
290.29 |
|
|
|
| 5 |
A' |
1426 |
1368 |
0.63 |
|
|
|
| 6 |
A' |
1369 |
1314 |
26.17 |
|
|
|
| 7 |
A' |
1144 |
1098 |
298.00 |
|
|
|
| 8 |
A' |
1101 |
1057 |
28.48 |
|
|
|
| 9 |
A' |
598 |
574 |
38.48 |
|
|
|
| 10 |
A" |
1086 |
1042 |
80.16 |
|
|
|
| 11 |
A" |
860 |
825 |
61.46 |
|
|
|
| 12 |
A" |
549 |
527 |
89.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10177.4 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 9766.2 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 HSEh1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.435 |
0.000 |
| O2 |
-1.097 |
-0.351 |
0.000 |
| N3 |
1.220 |
0.126 |
0.000 |
| H4 |
-0.304 |
1.480 |
0.000 |
| H5 |
-0.838 |
-1.280 |
0.000 |
| H6 |
1.376 |
-0.883 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3493 | 1.2588 | 1.0884 | 1.9086 | 1.9055 |
O2 | 1.3493 | | 2.3662 | 1.9947 | 0.9644 | 2.5299 | N3 | 1.2588 | 2.3662 | | 2.0388 | 2.4934 | 1.0216 | H4 | 1.0884 | 1.9947 | 2.0388 | | 2.8107 | 2.8996 | H5 | 1.9086 | 0.9644 | 2.4934 | 2.8107 | | 2.2499 | H6 | 1.9055 | 2.5299 | 1.0216 | 2.8996 | 2.2499 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
110.045 |
|
C1 |
N3 |
H6 |
112.942 |
| O2 |
C1 |
N3 |
130.224 |
|
O2 |
C1 |
H4 |
109.359 |
| N3 |
C1 |
H4 |
120.416 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.116 |
|
|
|
| 2 |
O |
-0.485 |
|
|
|
| 3 |
N |
-0.519 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
| 5 |
H |
0.387 |
|
|
|
| 6 |
H |
0.264 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.959 |
-2.050 |
0.000 |
2.263 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.122 |
-1.940 |
0.000 |
| y |
-1.940 |
-12.811 |
0.000 |
| z |
0.000 |
0.000 |
-18.737 |
|
| Traceless |
| | x | y | z |
| x |
-7.348 |
-1.940 |
0.000 |
| y |
-1.940 |
8.118 |
0.000 |
| z |
0.000 |
0.000 |
-0.770 |
|
| Polar |
| 3z2-r2 | -1.541 |
| x2-y2 | -10.311 |
| xy | -1.940 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.149 |
-0.146 |
0.000 |
| y |
-0.146 |
3.489 |
0.000 |
| z |
0.000 |
0.000 |
1.727 |
<r2> (average value of r
2) Å
2
| <r2> |
40.965 |
| (<r2>)1/2 |
6.400 |