Jump to
S1C2
S1C3
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -168.833597 |
| Energy at 298.15K | -168.837525 |
| HF Energy | -168.833597 |
| Nuclear repulsion energy | 70.149020 |
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 B1B95/3-21G
| 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' |
3601 |
3445 |
25.40 |
|
|
|
| 2 |
A' |
3449 |
3300 |
2.99 |
|
|
|
| 3 |
A' |
3035 |
2904 |
73.58 |
|
|
|
| 4 |
A' |
1795 |
1718 |
133.23 |
|
|
|
| 5 |
A' |
1443 |
1381 |
7.38 |
|
|
|
| 6 |
A' |
1286 |
1230 |
141.30 |
|
|
|
| 7 |
A' |
1182 |
1131 |
37.57 |
|
|
|
| 8 |
A' |
1005 |
962 |
309.18 |
|
|
|
| 9 |
A' |
621 |
594 |
2.22 |
|
|
|
| 10 |
A" |
1088 |
1041 |
3.32 |
|
|
|
| 11 |
A" |
839 |
803 |
80.74 |
|
|
|
| 12 |
A" |
339 |
324 |
86.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9841.4 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 9415.2 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.389 |
0.000 |
| O2 |
-1.003 |
-0.556 |
0.000 |
| N3 |
1.199 |
0.005 |
0.000 |
| H4 |
-0.364 |
1.422 |
0.000 |
| H5 |
-1.885 |
-0.115 |
0.000 |
| H6 |
1.880 |
0.772 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3780 | 1.2589 | 1.0950 | 1.9513 | 1.9190 |
O2 | 1.3780 | | 2.2726 | 2.0784 | 0.9858 | 3.1745 | N3 | 1.2589 | 2.2726 | | 2.1092 | 3.0865 | 1.0255 | H4 | 1.0950 | 2.0784 | 2.1092 | | 2.1627 | 2.3364 | H5 | 1.9513 | 0.9858 | 3.0865 | 2.1627 | | 3.8686 | H6 | 1.9190 | 3.1745 | 1.0255 | 2.3364 | 3.8686 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
110.174 |
|
C1 |
N3 |
H6 |
113.901 |
| O2 |
C1 |
N3 |
118.976 |
|
O2 |
C1 |
H4 |
113.885 |
| N3 |
C1 |
H4 |
127.139 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.297 |
|
|
|
| 2 |
O |
-0.548 |
|
|
|
| 3 |
N |
-0.571 |
|
|
|
| 4 |
H |
0.177 |
|
|
|
| 5 |
H |
0.370 |
|
|
|
| 6 |
H |
0.275 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.868 |
3.495 |
0.000 |
3.963 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.791 |
1.407 |
0.000 |
| y |
1.407 |
-17.916 |
0.000 |
| z |
0.000 |
0.000 |
-18.285 |
|
| Traceless |
| | x | y | z |
| x |
5.310 |
1.407 |
0.000 |
| y |
1.407 |
-2.378 |
0.000 |
| z |
0.000 |
0.000 |
-2.931 |
|
| Polar |
| 3z2-r2 | -5.863 |
| x2-y2 | 5.125 |
| xy | 1.407 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.665 |
0.087 |
0.000 |
| y |
0.087 |
2.432 |
0.000 |
| z |
0.000 |
0.000 |
0.940 |
<r2> (average value of r
2) Å
2
| <r2> |
41.546 |
| (<r2>)1/2 |
6.446 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -168.847300 |
| Energy at 298.15K | -168.851460 |
| HF Energy | -168.847300 |
| Nuclear repulsion energy | 70.512759 |
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 B1B95/3-21G
| 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' |
3520 |
3368 |
16.69 |
|
|
|
| 2 |
A' |
3459 |
3309 |
2.64 |
|
|
|
| 3 |
A' |
3150 |
3014 |
37.52 |
|
|
|
| 4 |
A' |
1746 |
1670 |
168.65 |
|
|
|
| 5 |
A' |
1409 |
1348 |
5.81 |
|
|
|
| 6 |
A' |
1395 |
1334 |
45.22 |
|
|
|
| 7 |
A' |
1162 |
1111 |
89.81 |
|
|
|
| 8 |
A' |
1030 |
985 |
213.72 |
|
|
|
| 9 |
A' |
573 |
548 |
56.78 |
|
|
|
| 10 |
A" |
1092 |
1045 |
1.23 |
|
|
|
| 11 |
A" |
835 |
799 |
48.47 |
|
|
|
| 12 |
A" |
667 |
638 |
238.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 10018.2 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 9584.4 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.431 |
0.000 |
| O2 |
-1.116 |
-0.360 |
0.000 |
| N3 |
1.159 |
-0.070 |
0.000 |
| H4 |
-0.304 |
1.475 |
0.000 |
| H5 |
-0.807 |
-1.304 |
0.000 |
| H6 |
1.927 |
0.608 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3683 | 1.2631 | 1.0870 | 1.9137 | 1.9352 |
O2 | 1.3683 | | 2.2941 | 2.0066 | 0.9940 | 3.1937 | N3 | 1.2631 | 2.2941 | | 2.1278 | 2.3211 | 1.0243 | H4 | 1.0870 | 2.0066 | 2.1278 | | 2.8242 | 2.3933 | H5 | 1.9137 | 0.9940 | 2.3211 | 2.8242 | | 3.3360 | H6 | 1.9352 | 3.1937 | 1.0243 | 2.3933 | 3.3360 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
107.150 |
|
C1 |
N3 |
H6 |
115.161 |
| O2 |
C1 |
N3 |
121.297 |
|
O2 |
C1 |
H4 |
109.090 |
| N3 |
C1 |
H4 |
129.614 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.296 |
|
|
|
| 2 |
O |
-0.560 |
|
|
|
| 3 |
N |
-0.615 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
| 5 |
H |
0.374 |
|
|
|
| 6 |
H |
0.280 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.550 |
0.979 |
0.000 |
1.123 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.061 |
3.358 |
0.000 |
| y |
3.358 |
-13.618 |
0.000 |
| z |
0.000 |
0.000 |
-18.282 |
|
| Traceless |
| | x | y | z |
| x |
-3.111 |
3.358 |
0.000 |
| y |
3.358 |
5.054 |
0.000 |
| z |
0.000 |
0.000 |
-1.943 |
|
| Polar |
| 3z2-r2 | -3.885 |
| x2-y2 | -5.443 |
| xy | 3.358 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.958 |
0.184 |
0.000 |
| y |
0.184 |
2.936 |
0.000 |
| z |
0.000 |
0.000 |
0.940 |
<r2> (average value of r
2) Å
2
| <r2> |
40.878 |
| (<r2>)1/2 |
6.394 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -168.842735 |
| Energy at 298.15K | -168.846815 |
| HF Energy | -168.842735 |
| Nuclear repulsion energy | 69.906507 |
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 B1B95/3-21G
| 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' |
3536 |
3383 |
5.11 |
|
|
|
| 2 |
A' |
3365 |
3219 |
8.87 |
|
|
|
| 3 |
A' |
3233 |
3093 |
11.63 |
|
|
|
| 4 |
A' |
1735 |
1660 |
161.03 |
|
|
|
| 5 |
A' |
1434 |
1372 |
0.48 |
|
|
|
| 6 |
A' |
1337 |
1279 |
16.23 |
|
|
|
| 7 |
A' |
1109 |
1061 |
268.11 |
|
|
|
| 8 |
A' |
1041 |
996 |
112.72 |
|
|
|
| 9 |
A' |
575 |
550 |
36.86 |
|
|
|
| 10 |
A" |
1107 |
1059 |
88.28 |
|
|
|
| 11 |
A" |
860 |
823 |
57.63 |
|
|
|
| 12 |
A" |
527 |
504 |
120.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9929.2 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 9499.2 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.440 |
0.000 |
| O2 |
-1.113 |
-0.380 |
0.000 |
| N3 |
1.231 |
0.159 |
0.000 |
| H4 |
-0.334 |
1.469 |
0.000 |
| H5 |
-0.848 |
-1.336 |
0.000 |
| H6 |
1.463 |
-0.847 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
H4 |
H5 |
H6 |
| C1 | | 1.3826 | 1.2631 | 1.0813 | 1.9683 | 1.9482 |
O2 | 1.3826 | | 2.4053 | 2.0066 | 0.9911 | 2.6170 | N3 | 1.2631 | 2.4053 | | 2.0409 | 2.5612 | 1.0320 | H4 | 1.0813 | 2.0066 | 2.0409 | | 2.8514 | 2.9306 | H5 | 1.9683 | 0.9911 | 2.5612 | 2.8514 | | 2.3621 | H6 | 1.9482 | 2.6170 | 1.0320 | 2.9306 | 2.3621 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H5 |
110.960 |
|
C1 |
N3 |
H6 |
115.809 |
| O2 |
C1 |
N3 |
130.714 |
|
O2 |
C1 |
H4 |
108.440 |
| N3 |
C1 |
H4 |
120.846 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.257 |
|
|
|
| 2 |
O |
-0.551 |
|
|
|
| 3 |
N |
-0.577 |
|
|
|
| 4 |
H |
0.257 |
|
|
|
| 5 |
H |
0.358 |
|
|
|
| 6 |
H |
0.257 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.601 |
-2.239 |
0.000 |
2.318 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.730 |
-2.278 |
0.000 |
| y |
-2.278 |
-12.691 |
0.000 |
| z |
0.000 |
0.000 |
-18.318 |
|
| Traceless |
| | x | y | z |
| x |
-7.225 |
-2.278 |
0.000 |
| y |
-2.278 |
7.833 |
0.000 |
| z |
0.000 |
0.000 |
-0.607 |
|
| Polar |
| 3z2-r2 | -1.215 |
| x2-y2 | -10.039 |
| xy | -2.278 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.687 |
-0.181 |
0.000 |
| y |
-0.181 |
3.168 |
0.000 |
| z |
0.000 |
0.000 |
1.006 |
<r2> (average value of r
2) Å
2
| <r2> |
41.833 |
| (<r2>)1/2 |
6.468 |