Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -135.106020 |
| Energy at 298.15K | -135.114143 |
| Nuclear repulsion energy | 82.865245 |
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 B1B95/6-31+G**
| 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' |
3535 |
3382 |
0.74 |
|
|
|
| 2 |
A' |
3126 |
2991 |
43.74 |
|
|
|
| 3 |
A' |
3062 |
2929 |
36.64 |
|
|
|
| 4 |
A' |
3044 |
2912 |
27.41 |
|
|
|
| 5 |
A' |
1668 |
1595 |
32.28 |
|
|
|
| 6 |
A' |
1502 |
1437 |
3.79 |
|
|
|
| 7 |
A' |
1485 |
1421 |
0.17 |
|
|
|
| 8 |
A' |
1408 |
1347 |
15.40 |
|
|
|
| 9 |
A' |
1375 |
1315 |
12.79 |
|
|
|
| 10 |
A' |
1153 |
1103 |
12.73 |
|
|
|
| 11 |
A' |
1083 |
1036 |
29.53 |
|
|
|
| 12 |
A' |
894 |
856 |
4.55 |
|
|
|
| 13 |
A' |
835 |
799 |
193.28 |
|
|
|
| 14 |
A' |
399 |
382 |
8.76 |
|
|
|
| 15 |
A" |
3628 |
3471 |
1.33 |
|
|
|
| 16 |
A" |
3131 |
2995 |
58.54 |
|
|
|
| 17 |
A" |
3099 |
2964 |
5.67 |
|
|
|
| 18 |
A" |
1493 |
1428 |
9.62 |
|
|
|
| 19 |
A" |
1385 |
1325 |
0.11 |
|
|
|
| 20 |
A" |
1264 |
1209 |
0.00 |
|
|
|
| 21 |
A" |
1001 |
958 |
1.20 |
|
|
|
| 22 |
A" |
773 |
739 |
1.03 |
|
|
|
| 23 |
A" |
290 |
277 |
38.82 |
|
|
|
| 24 |
A" |
250 |
239 |
18.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20440.6 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 19553.5 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.302 |
-0.084 |
0.000 |
| C2 |
0.000 |
0.569 |
0.000 |
| C3 |
1.213 |
-0.356 |
0.000 |
| H4 |
2.148 |
0.212 |
0.000 |
| H5 |
1.214 |
-1.002 |
0.884 |
| H6 |
1.214 |
-1.002 |
-0.884 |
| H7 |
0.038 |
1.228 |
-0.874 |
| H8 |
0.038 |
1.228 |
0.874 |
| H9 |
-1.408 |
-0.678 |
0.816 |
| H10 |
-1.408 |
-0.678 |
-0.816 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4569 | 2.5298 | 3.4633 | 2.8202 | 2.8202 | 2.0692 | 2.0692 | 1.0142 | 1.0142 |
C2 | 1.4569 | | 1.5257 | 2.1779 | 2.1733 | 2.1733 | 1.0948 | 1.0948 | 2.0501 | 2.0501 | C3 | 2.5298 | 1.5257 | | 1.0947 | 1.0946 | 1.0946 | 2.1567 | 2.1567 | 2.7638 | 2.7638 | H4 | 3.4633 | 2.1779 | 1.0947 | | 1.7690 | 1.7690 | 2.4993 | 2.4993 | 3.7558 | 3.7558 | H5 | 2.8202 | 2.1733 | 1.0946 | 1.7690 | | 1.7677 | 3.0728 | 2.5203 | 2.6427 | 3.1413 | H6 | 2.8202 | 2.1733 | 1.0946 | 1.7690 | 1.7677 | | 2.5203 | 3.0728 | 3.1413 | 2.6427 | H7 | 2.0692 | 1.0948 | 2.1567 | 2.4993 | 3.0728 | 2.5203 | | 1.7480 | 2.9286 | 2.3928 | H8 | 2.0692 | 1.0948 | 2.1567 | 2.4993 | 2.5203 | 3.0728 | 1.7480 | | 2.3928 | 2.9286 | H9 | 1.0142 | 2.0501 | 2.7638 | 3.7558 | 2.6427 | 3.1413 | 2.9286 | 2.3928 | | 1.6311 | H10 | 1.0142 | 2.0501 | 2.7638 | 3.7558 | 3.1413 | 2.6427 | 2.3928 | 2.9286 | 1.6311 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.008 |
|
N1 |
C2 |
H7 |
107.521 |
| N1 |
C2 |
H8 |
107.521 |
|
C2 |
N1 |
H9 |
110.846 |
| C2 |
N1 |
H10 |
110.846 |
|
C2 |
C3 |
H4 |
111.369 |
| C2 |
C3 |
H5 |
111.003 |
|
C2 |
C3 |
H6 |
111.003 |
| C3 |
C2 |
H7 |
109.679 |
|
C3 |
C2 |
H8 |
109.679 |
| H4 |
C3 |
H5 |
107.804 |
|
H4 |
C3 |
H6 |
107.804 |
| H5 |
C3 |
H6 |
107.695 |
|
H7 |
C2 |
H8 |
105.941 |
| H9 |
N1 |
H10 |
107.058 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.619 |
|
|
|
| 2 |
C |
-0.212 |
|
|
|
| 3 |
C |
-0.517 |
|
|
|
| 4 |
H |
0.156 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
| 6 |
H |
0.154 |
|
|
|
| 7 |
H |
0.154 |
|
|
|
| 8 |
H |
0.154 |
|
|
|
| 9 |
H |
0.287 |
|
|
|
| 10 |
H |
0.287 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.042 |
-0.986 |
0.000 |
1.434 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.468 |
2.864 |
0.000 |
| y |
2.864 |
-20.627 |
0.000 |
| z |
0.000 |
0.000 |
-19.160 |
|
| Traceless |
| | x | y | z |
| x |
-4.574 |
2.864 |
0.000 |
| y |
2.864 |
1.187 |
0.000 |
| z |
0.000 |
0.000 |
3.388 |
|
| Polar |
| 3z2-r2 | 6.775 |
| x2-y2 | -3.841 |
| xy | 2.864 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.670 |
-0.039 |
0.000 |
| y |
-0.039 |
5.036 |
0.000 |
| z |
0.000 |
0.000 |
4.692 |
<r2> (average value of r
2) Å
2
| <r2> |
58.766 |
| (<r2>)1/2 |
7.666 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -135.105338 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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 B1B95/6-31+G**
Geometric Data calculated at B1B95/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability