Jump to
S1C2
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -207.932363 |
| Energy at 298.15K | -207.938580 |
| Nuclear repulsion energy | 118.848418 |
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 |
4200 |
3798 |
92.39 |
|
|
|
| 2 |
A |
3294 |
2979 |
39.33 |
|
|
|
| 3 |
A |
3279 |
2966 |
1.34 |
|
|
|
| 4 |
A |
3186 |
2881 |
29.70 |
|
|
|
| 5 |
A |
1953 |
1766 |
10.32 |
|
|
|
| 6 |
A |
1620 |
1465 |
17.93 |
|
|
|
| 7 |
A |
1600 |
1447 |
26.47 |
|
|
|
| 8 |
A |
1541 |
1394 |
25.48 |
|
|
|
| 9 |
A |
1433 |
1296 |
61.96 |
|
|
|
| 10 |
A |
1251 |
1132 |
8.81 |
|
|
|
| 11 |
A |
1159 |
1048 |
146.03 |
|
|
|
| 12 |
A |
992 |
897 |
2.43 |
|
|
|
| 13 |
A |
614 |
555 |
15.66 |
|
|
|
| 14 |
A |
354 |
320 |
2.11 |
|
|
|
| 15 |
A |
3233 |
2924 |
35.53 |
|
|
|
| 16 |
A |
1613 |
1459 |
9.17 |
|
|
|
| 17 |
A |
1202 |
1087 |
2.71 |
|
|
|
| 18 |
A |
1007 |
911 |
9.17 |
|
|
|
| 19 |
A |
394 |
356 |
184.87 |
|
|
|
| 20 |
A |
320 |
290 |
4.81 |
|
|
|
| 21 |
A |
208 |
188 |
0.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17225.9 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15579.1 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 |
-1.298 |
1.291 |
0.000 |
| C2 |
0.000 |
0.547 |
0.000 |
| N3 |
0.021 |
-0.701 |
0.000 |
| O4 |
1.297 |
-1.194 |
0.000 |
| H5 |
1.198 |
-2.127 |
0.000 |
| H6 |
-2.130 |
0.602 |
0.000 |
| H7 |
-1.369 |
1.930 |
0.875 |
| H8 |
-1.369 |
1.930 |
-0.875 |
| H9 |
0.929 |
1.100 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4960 | 2.3887 | 3.5933 | 4.2326 | 1.0812 | 1.0855 | 1.0855 | 2.2350 |
C2 | 1.4960 | | 1.2475 | 2.1713 | 2.9301 | 2.1310 | 2.1337 | 2.1337 | 1.0814 | N3 | 2.3887 | 1.2475 | | 1.3686 | 1.8496 | 2.5147 | 3.1013 | 3.1013 | 2.0165 | O4 | 3.5933 | 2.1713 | 1.3686 | | 0.9381 | 3.8697 | 4.1996 | 4.1996 | 2.3234 | H5 | 4.2326 | 2.9301 | 1.8496 | 0.9381 | | 4.3042 | 4.8803 | 4.8803 | 3.2381 | H6 | 1.0812 | 2.1310 | 2.5147 | 3.8697 | 4.3042 | | 1.7635 | 1.7635 | 3.0998 | H7 | 1.0855 | 2.1337 | 3.1013 | 4.1996 | 4.8803 | 1.7635 | | 1.7492 | 2.5953 | H8 | 1.0855 | 2.1337 | 3.1013 | 4.1996 | 4.8803 | 1.7635 | 1.7492 | | 2.5953 | H9 | 2.2350 | 1.0814 | 2.0165 | 2.3234 | 3.2381 | 3.0998 | 2.5953 | 2.5953 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.811 |
|
C1 |
C2 |
H9 |
119.391 |
| C2 |
C1 |
H6 |
110.522 |
|
C2 |
C1 |
H7 |
110.484 |
| C2 |
C1 |
H8 |
110.484 |
|
C2 |
N3 |
O4 |
112.106 |
| N3 |
C2 |
H9 |
119.798 |
|
N3 |
O4 |
H5 |
105.080 |
| H6 |
C1 |
H7 |
108.960 |
|
H6 |
C1 |
H8 |
108.960 |
| H7 |
C1 |
H8 |
107.354 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.572 |
-0.345 |
|
-0.492 |
| 2 |
H |
0.439 |
0.454 |
|
0.450 |
| 3 |
N |
-0.127 |
-0.382 |
|
-0.369 |
| 4 |
C |
0.034 |
-0.519 |
|
-0.537 |
| 5 |
H |
0.209 |
0.476 |
|
0.489 |
| 6 |
C |
-0.665 |
0.099 |
|
0.141 |
| 7 |
H |
0.239 |
0.090 |
|
0.132 |
| 8 |
H |
0.222 |
0.090 |
|
0.132 |
| 9 |
H |
0.222 |
0.037 |
|
0.055 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.469 |
0.634 |
0.000 |
0.788 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.436 |
0.600 |
0.000 |
0.742 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.852 |
-1.996 |
0.000 |
| y |
-1.996 |
-18.496 |
0.000 |
| z |
0.000 |
0.000 |
-25.181 |
|
| Traceless |
| | x | y | z |
| x |
-4.014 |
-1.996 |
0.000 |
| y |
-1.996 |
7.021 |
0.000 |
| z |
0.000 |
0.000 |
-3.007 |
|
| Polar |
| 3z2-r2 | -6.014 |
| x2-y2 | -7.356 |
| xy | -1.996 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.767 |
-1.167 |
0.000 |
| y |
-1.167 |
6.509 |
0.000 |
| z |
0.000 |
0.000 |
3.119 |
<r2> (average value of r
2) Å
2
| <r2> |
90.354 |
| (<r2>)1/2 |
9.505 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -207.931108 |
| Energy at 298.15K | -207.937288 |
| HF Energy | -207.931108 |
| Nuclear repulsion energy | 121.290970 |
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' |
4203 |
3801 |
96.92 |
|
|
|
| 2 |
A' |
3333 |
3015 |
28.99 |
|
|
|
| 3 |
A' |
3319 |
3002 |
2.19 |
|
|
|
| 4 |
A' |
3190 |
2885 |
24.22 |
|
|
|
| 5 |
A' |
1961 |
1774 |
17.86 |
|
|
|
| 6 |
A' |
1616 |
1462 |
23.44 |
|
|
|
| 7 |
A' |
1551 |
1403 |
26.58 |
|
|
|
| 8 |
A' |
1539 |
1392 |
60.83 |
|
|
|
| 9 |
A' |
1487 |
1345 |
27.25 |
|
|
|
| 10 |
A' |
1246 |
1127 |
12.95 |
|
|
|
| 11 |
A' |
1088 |
984 |
140.31 |
|
|
|
| 12 |
A' |
973 |
880 |
0.60 |
|
|
|
| 13 |
A' |
731 |
661 |
15.57 |
|
|
|
| 14 |
A' |
337 |
305 |
1.79 |
|
|
|
| 15 |
A" |
3233 |
2924 |
32.51 |
|
|
|
| 16 |
A" |
1624 |
1468 |
10.93 |
|
|
|
| 17 |
A" |
1189 |
1075 |
1.52 |
|
|
|
| 18 |
A" |
969 |
876 |
7.65 |
|
|
|
| 19 |
A" |
534 |
483 |
23.50 |
|
|
|
| 20 |
A" |
402 |
364 |
157.27 |
|
|
|
| 21 |
A" |
53 |
48 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17288.5 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15635.7 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 |
-1.452 |
0.471 |
0.000 |
| C2 |
0.000 |
0.845 |
0.000 |
| N3 |
0.997 |
0.090 |
0.000 |
| O4 |
0.680 |
-1.241 |
0.000 |
| H5 |
1.507 |
-1.683 |
0.000 |
| H6 |
-1.593 |
-0.597 |
0.000 |
| H7 |
-1.938 |
0.894 |
0.874 |
| H8 |
-1.938 |
0.894 |
-0.874 |
| H9 |
0.253 |
1.892 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4990 | 2.4785 | 2.7339 | 3.6597 | 1.0775 | 1.0856 | 1.0856 | 2.2194 |
C2 | 1.4990 | | 1.2504 | 2.1934 | 2.9424 | 2.1488 | 2.1265 | 2.1265 | 1.0778 | N3 | 2.4785 | 1.2504 | | 1.3684 | 1.8447 | 2.6804 | 3.1663 | 3.1663 | 1.9497 | O4 | 2.7339 | 2.1934 | 1.3684 | | 0.9378 | 2.3627 | 3.4889 | 3.4889 | 3.1620 | H5 | 3.6597 | 2.9424 | 1.8447 | 0.9378 | | 3.2851 | 4.3897 | 4.3897 | 3.7885 | H6 | 1.0775 | 2.1488 | 2.6804 | 2.3627 | 3.2851 | | 1.7619 | 1.7619 | 3.0993 | H7 | 1.0856 | 2.1265 | 3.1663 | 3.4889 | 4.3897 | 1.7619 | | 1.7475 | 2.5615 | H8 | 1.0856 | 2.1265 | 3.1663 | 3.4889 | 4.3897 | 1.7619 | 1.7475 | | 2.5615 | H9 | 2.2194 | 1.0778 | 1.9497 | 3.1620 | 3.7885 | 3.0993 | 2.5615 | 2.5615 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.474 |
|
C1 |
C2 |
H9 |
117.995 |
| C2 |
C1 |
H6 |
111.980 |
|
C2 |
C1 |
H7 |
109.689 |
| C2 |
C1 |
H8 |
109.689 |
|
C2 |
N3 |
O4 |
113.686 |
| N3 |
C2 |
H9 |
113.531 |
|
N3 |
O4 |
H5 |
104.695 |
| H6 |
C1 |
H7 |
109.080 |
|
H6 |
C1 |
H8 |
109.080 |
| H7 |
C1 |
H8 |
107.202 |
|
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 |
-0.687 |
|
|
|
| 2 |
C |
0.011 |
|
|
|
| 3 |
N |
-0.119 |
|
|
|
| 4 |
O |
-0.585 |
|
|
|
| 5 |
H |
0.443 |
|
|
|
| 6 |
H |
0.268 |
|
|
|
| 7 |
H |
0.224 |
|
|
|
| 8 |
H |
0.224 |
|
|
|
| 9 |
H |
0.221 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.623 |
0.358 |
0.000 |
0.719 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.939 |
-4.123 |
0.000 |
| y |
-4.123 |
-21.252 |
0.000 |
| z |
0.000 |
0.000 |
-25.204 |
|
| Traceless |
| | x | y | z |
| x |
0.290 |
-4.123 |
0.000 |
| y |
-4.123 |
2.819 |
0.000 |
| z |
0.000 |
0.000 |
-3.109 |
|
| Polar |
| 3z2-r2 | -6.217 |
| x2-y2 | -1.686 |
| xy | -4.123 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.382 |
-1.276 |
0.000 |
| y |
-1.276 |
5.542 |
0.000 |
| z |
0.000 |
0.000 |
3.129 |
<r2> (average value of r
2) Å
2
| <r2> |
78.017 |
| (<r2>)1/2 |
8.833 |