Jump to
S1C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -207.945339 |
| Energy at 298.15K | -207.951557 |
| Nuclear repulsion energy | 118.834407 |
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 |
3816 |
131.01 |
|
|
|
| 2 |
A |
3274 |
2974 |
31.14 |
|
|
|
| 3 |
A |
3259 |
2961 |
2.00 |
|
|
|
| 4 |
A |
3168 |
2878 |
25.44 |
|
|
|
| 5 |
A |
1946 |
1768 |
9.10 |
|
|
|
| 6 |
A |
1601 |
1455 |
14.56 |
|
|
|
| 7 |
A |
1578 |
1433 |
19.35 |
|
|
|
| 8 |
A |
1524 |
1385 |
25.37 |
|
|
|
| 9 |
A |
1417 |
1287 |
63.77 |
|
|
|
| 10 |
A |
1245 |
1131 |
9.56 |
|
|
|
| 11 |
A |
1157 |
1051 |
147.16 |
|
|
|
| 12 |
A |
988 |
898 |
1.80 |
|
|
|
| 13 |
A |
613 |
557 |
14.82 |
|
|
|
| 14 |
A |
353 |
321 |
2.26 |
|
|
|
| 15 |
A |
3218 |
2924 |
30.19 |
|
|
|
| 16 |
A |
1597 |
1451 |
9.20 |
|
|
|
| 17 |
A |
1197 |
1088 |
2.98 |
|
|
|
| 18 |
A |
1006 |
914 |
9.18 |
|
|
|
| 19 |
A |
383 |
348 |
160.54 |
|
|
|
| 20 |
A |
320 |
291 |
5.86 |
|
|
|
| 21 |
A |
211 |
192 |
0.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17127.9 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 15560.7 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 |
-1.299 |
1.290 |
0.000 |
| C2 |
0.000 |
0.547 |
0.000 |
| N3 |
0.022 |
-0.700 |
0.000 |
| O4 |
1.299 |
-1.194 |
0.000 |
| H5 |
1.190 |
-2.127 |
0.000 |
| H6 |
-2.129 |
0.596 |
0.000 |
| H7 |
-1.368 |
1.928 |
0.876 |
| H8 |
-1.368 |
1.928 |
-0.876 |
| H9 |
0.928 |
1.104 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4961 | 2.3883 | 3.5936 | 4.2266 | 1.0820 | 1.0864 | 1.0864 | 2.2350 |
C2 | 1.4961 | | 1.2478 | 2.1720 | 2.9267 | 2.1298 | 2.1321 | 2.1321 | 1.0823 | N3 | 2.3883 | 1.2478 | | 1.3688 | 1.8435 | 2.5112 | 3.0996 | 3.0996 | 2.0190 | O4 | 3.5936 | 2.1720 | 1.3688 | | 0.9393 | 3.8666 | 4.1981 | 4.1981 | 2.3272 | H5 | 4.2266 | 2.9267 | 1.8435 | 0.9393 | | 4.2925 | 4.8735 | 4.8735 | 3.2411 | H6 | 1.0820 | 2.1298 | 2.5112 | 3.8666 | 4.2925 | | 1.7672 | 1.7672 | 3.0994 | H7 | 1.0864 | 2.1321 | 3.0996 | 4.1981 | 4.8735 | 1.7672 | | 1.7524 | 2.5922 | H8 | 1.0864 | 2.1321 | 3.0996 | 4.1981 | 4.8735 | 1.7672 | 1.7524 | | 2.5922 | H9 | 2.2350 | 1.0823 | 2.0190 | 2.3272 | 3.2411 | 3.0994 | 2.5922 | 2.5922 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
120.743 |
|
C1 |
C2 |
H9 |
119.314 |
| C2 |
C1 |
H6 |
110.365 |
|
C2 |
C1 |
H7 |
110.288 |
| C2 |
C1 |
H8 |
110.288 |
|
C2 |
N3 |
O4 |
112.136 |
| N3 |
C2 |
H9 |
119.943 |
|
N3 |
O4 |
H5 |
104.474 |
| H6 |
C1 |
H7 |
109.164 |
|
H6 |
C1 |
H8 |
109.164 |
| H7 |
C1 |
H8 |
107.515 |
|
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 |
-0.239 |
|
|
|
| 2 |
C |
0.073 |
|
|
|
| 3 |
N |
-0.149 |
|
|
|
| 4 |
O |
-0.376 |
|
|
|
| 5 |
H |
0.268 |
|
|
|
| 6 |
H |
0.118 |
|
|
|
| 7 |
H |
0.104 |
|
|
|
| 8 |
H |
0.104 |
|
|
|
| 9 |
H |
0.098 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.453 |
0.727 |
0.000 |
0.857 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.672 |
-1.927 |
0.000 |
| y |
-1.927 |
-18.697 |
0.000 |
| z |
0.000 |
0.000 |
-25.066 |
|
| Traceless |
| | x | y | z |
| x |
-3.791 |
-1.927 |
0.000 |
| y |
-1.927 |
6.672 |
0.000 |
| z |
0.000 |
0.000 |
-2.881 |
|
| Polar |
| 3z2-r2 | -5.762 |
| x2-y2 | -6.975 |
| xy | -1.927 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.864 |
-1.177 |
0.000 |
| y |
-1.177 |
6.581 |
0.000 |
| z |
0.000 |
0.000 |
3.220 |
<r2> (average value of r
2) Å
2
| <r2> |
90.300 |
| (<r2>)1/2 |
9.503 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -207.944082 |
| Energy at 298.15K | -207.950281 |
| HF Energy | -207.944082 |
| Nuclear repulsion energy | 121.289735 |
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' |
4204 |
3819 |
136.25 |
|
|
|
| 2 |
A' |
3314 |
3011 |
20.32 |
|
|
|
| 3 |
A' |
3299 |
2997 |
4.15 |
|
|
|
| 4 |
A' |
3172 |
2882 |
20.56 |
|
|
|
| 5 |
A' |
1954 |
1776 |
17.08 |
|
|
|
| 6 |
A' |
1597 |
1451 |
19.19 |
|
|
|
| 7 |
A' |
1535 |
1395 |
12.15 |
|
|
|
| 8 |
A' |
1511 |
1373 |
67.25 |
|
|
|
| 9 |
A' |
1476 |
1341 |
30.37 |
|
|
|
| 10 |
A' |
1239 |
1125 |
13.34 |
|
|
|
| 11 |
A' |
1087 |
988 |
141.14 |
|
|
|
| 12 |
A' |
971 |
882 |
0.83 |
|
|
|
| 13 |
A' |
730 |
663 |
14.78 |
|
|
|
| 14 |
A' |
339 |
308 |
1.66 |
|
|
|
| 15 |
A" |
3219 |
2925 |
27.17 |
|
|
|
| 16 |
A" |
1608 |
1460 |
10.43 |
|
|
|
| 17 |
A" |
1183 |
1075 |
1.64 |
|
|
|
| 18 |
A" |
968 |
879 |
7.47 |
|
|
|
| 19 |
A" |
532 |
484 |
18.14 |
|
|
|
| 20 |
A" |
391 |
356 |
139.71 |
|
|
|
| 21 |
A" |
64 |
59 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17196.9 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 15623.4 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 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 |
0.679 |
-1.241 |
0.000 |
| H5 |
1.511 |
-1.675 |
0.000 |
| H6 |
-1.591 |
-0.599 |
0.000 |
| H7 |
-1.936 |
0.895 |
0.875 |
| H8 |
-1.936 |
0.895 |
-0.875 |
| H9 |
0.252 |
1.893 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4993 | 2.4786 | 2.7329 | 3.6586 | 1.0785 | 1.0864 | 1.0864 | 2.2197 |
C2 | 1.4993 | | 1.2507 | 2.1932 | 2.9383 | 2.1479 | 2.1249 | 2.1249 | 1.0784 | N3 | 2.4786 | 1.2507 | | 1.3683 | 1.8384 | 2.6779 | 3.1648 | 3.1648 | 1.9513 | O4 | 2.7329 | 2.1932 | 1.3683 | | 0.9391 | 2.3582 | 3.4875 | 3.4875 | 3.1630 | H5 | 3.6586 | 2.9383 | 1.8384 | 0.9391 | | 3.2832 | 4.3878 | 4.3878 | 3.7841 | H6 | 1.0785 | 2.1479 | 2.6779 | 2.3582 | 3.2832 | | 1.7656 | 1.7656 | 3.0993 | H7 | 1.0864 | 2.1249 | 3.1648 | 3.4875 | 4.3878 | 1.7656 | | 1.7508 | 2.5589 | H8 | 1.0864 | 2.1249 | 3.1648 | 3.4875 | 4.3878 | 1.7656 | 1.7508 | | 2.5589 | H9 | 2.2197 | 1.0784 | 1.9513 | 3.1630 | 3.7841 | 3.0993 | 2.5589 | 2.5589 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.436 |
|
C1 |
C2 |
H9 |
117.959 |
| C2 |
C1 |
H6 |
111.825 |
|
C2 |
C1 |
H7 |
109.488 |
| C2 |
C1 |
H8 |
109.488 |
|
C2 |
N3 |
O4 |
113.656 |
| N3 |
C2 |
H9 |
113.604 |
|
N3 |
O4 |
H5 |
104.085 |
| H6 |
C1 |
H7 |
109.281 |
|
H6 |
C1 |
H8 |
109.281 |
| H7 |
C1 |
H8 |
107.371 |
|
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 |
-0.257 |
|
|
|
| 2 |
C |
0.045 |
|
|
|
| 3 |
N |
-0.139 |
|
|
|
| 4 |
O |
-0.391 |
|
|
|
| 5 |
H |
0.275 |
|
|
|
| 6 |
H |
0.141 |
|
|
|
| 7 |
H |
0.107 |
|
|
|
| 8 |
H |
0.107 |
|
|
|
| 9 |
H |
0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.726 |
0.381 |
0.000 |
0.820 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.978 |
-3.970 |
0.000 |
| y |
-3.970 |
-21.306 |
0.000 |
| z |
0.000 |
0.000 |
-25.089 |
|
| Traceless |
| | x | y | z |
| x |
0.220 |
-3.970 |
0.000 |
| y |
-3.970 |
2.727 |
0.000 |
| z |
0.000 |
0.000 |
-2.947 |
|
| Polar |
| 3z2-r2 | -5.894 |
| x2-y2 | -1.672 |
| xy | -3.970 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.482 |
-1.265 |
0.000 |
| y |
-1.265 |
5.607 |
0.000 |
| z |
0.000 |
0.000 |
3.233 |
<r2> (average value of r
2) Å
2
| <r2> |
77.976 |
| (<r2>)1/2 |
8.830 |