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S1C2
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -134.192793 |
| Energy at 298.15K | -134.200967 |
| Nuclear repulsion energy | 83.007330 |
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/6-31G
| 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 |
3423 |
0.79 |
|
|
|
| 2 |
A' |
3248 |
2933 |
69.15 |
|
|
|
| 3 |
A' |
3203 |
2892 |
35.59 |
|
|
|
| 4 |
A' |
3176 |
2868 |
35.40 |
|
|
|
| 5 |
A' |
1844 |
1665 |
36.56 |
|
|
|
| 6 |
A' |
1664 |
1502 |
3.62 |
|
|
|
| 7 |
A' |
1649 |
1489 |
0.36 |
|
|
|
| 8 |
A' |
1571 |
1419 |
4.96 |
|
|
|
| 9 |
A' |
1532 |
1383 |
11.94 |
|
|
|
| 10 |
A' |
1248 |
1127 |
22.46 |
|
|
|
| 11 |
A' |
1152 |
1040 |
32.18 |
|
|
|
| 12 |
A' |
961 |
868 |
4.04 |
|
|
|
| 13 |
A' |
640 |
578 |
371.14 |
|
|
|
| 14 |
A' |
435 |
393 |
25.48 |
|
|
|
| 15 |
A" |
3910 |
3531 |
4.35 |
|
|
|
| 16 |
A" |
3259 |
2942 |
98.47 |
|
|
|
| 17 |
A" |
3229 |
2915 |
0.01 |
|
|
|
| 18 |
A" |
1650 |
1490 |
6.32 |
|
|
|
| 19 |
A" |
1503 |
1357 |
0.48 |
|
|
|
| 20 |
A" |
1393 |
1258 |
0.68 |
|
|
|
| 21 |
A" |
1082 |
977 |
0.00 |
|
|
|
| 22 |
A" |
852 |
770 |
1.86 |
|
|
|
| 23 |
A" |
282 |
254 |
16.08 |
|
|
|
| 24 |
A" |
251 |
226 |
39.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21762.1 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 19649.0 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/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.282 |
-0.114 |
0.000 |
| C2 |
0.000 |
0.570 |
0.000 |
| C3 |
1.226 |
-0.350 |
0.000 |
| H4 |
2.147 |
0.223 |
0.000 |
| H5 |
1.228 |
-0.989 |
0.877 |
| H6 |
1.228 |
-0.989 |
-0.877 |
| H7 |
0.032 |
1.219 |
-0.867 |
| H8 |
0.032 |
1.219 |
0.867 |
| H9 |
-1.524 |
-0.604 |
0.831 |
| H10 |
-1.524 |
-0.604 |
-0.831 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4533 | 2.5190 | 3.4460 | 2.7999 | 2.7999 | 2.0634 | 2.0634 | 0.9949 | 0.9949 |
C2 | 1.4533 | | 1.5326 | 2.1751 | 2.1702 | 2.1702 | 1.0838 | 1.0838 | 2.0957 | 2.0957 | C3 | 2.5190 | 1.5326 | | 1.0854 | 1.0854 | 1.0854 | 2.1537 | 2.1537 | 2.8835 | 2.8835 | H4 | 3.4460 | 2.1751 | 1.0854 | | 1.7561 | 1.7561 | 2.4933 | 2.4933 | 3.8538 | 3.8538 | H5 | 2.7999 | 2.1702 | 1.0854 | 1.7561 | | 1.7544 | 3.0579 | 2.5115 | 2.7792 | 3.2620 | H6 | 2.7999 | 2.1702 | 1.0854 | 1.7561 | 1.7544 | | 2.5115 | 3.0579 | 3.2620 | 2.7792 | H7 | 2.0634 | 1.0838 | 2.1537 | 2.4933 | 3.0579 | 2.5115 | | 1.7345 | 2.9380 | 2.3976 | H8 | 2.0634 | 1.0838 | 2.1537 | 2.4933 | 2.5115 | 3.0579 | 1.7345 | | 2.3976 | 2.9380 | H9 | 0.9949 | 2.0957 | 2.8835 | 3.8538 | 2.7792 | 3.2620 | 2.9380 | 2.3976 | | 1.6625 | H10 | 0.9949 | 2.0957 | 2.8835 | 3.8538 | 3.2620 | 2.7792 | 2.3976 | 2.9380 | 1.6625 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.027 |
|
N1 |
C2 |
H7 |
107.958 |
| N1 |
C2 |
H8 |
107.958 |
|
C2 |
N1 |
H9 |
116.497 |
| C2 |
N1 |
H10 |
116.497 |
|
C2 |
C3 |
H4 |
111.219 |
| C2 |
C3 |
H5 |
110.831 |
|
C2 |
C3 |
H6 |
110.831 |
| C3 |
C2 |
H7 |
109.612 |
|
C3 |
C2 |
H8 |
109.612 |
| H4 |
C3 |
H5 |
107.992 |
|
H4 |
C3 |
H6 |
107.992 |
| H5 |
C3 |
H6 |
107.843 |
|
H7 |
C2 |
H8 |
106.302 |
| H9 |
N1 |
H10 |
113.331 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.851 |
-0.343 |
|
|
| 2 |
C |
-0.094 |
0.040 |
|
|
| 3 |
C |
-0.451 |
0.089 |
|
|
| 4 |
H |
0.146 |
0.091 |
|
|
| 5 |
H |
0.144 |
-1.283 |
|
|
| 6 |
H |
0.144 |
-0.064 |
|
|
| 7 |
H |
0.162 |
-0.119 |
|
|
| 8 |
H |
0.162 |
0.702 |
|
|
| 9 |
H |
0.319 |
0.441 |
|
|
| 10 |
H |
0.319 |
0.446 |
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.742 |
-0.952 |
0.000 |
1.207 |
| CHELPG |
0.354 |
0.531 |
1.018 |
1.201 |
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.458 |
-0.096 |
-0.120 |
| y |
-0.096 |
4.067 |
-0.212 |
| z |
-0.120 |
-0.212 |
3.672 |
<r2> (average value of r
2) Å
2
| <r2> |
58.823 |
| (<r2>)1/2 |
7.670 |
Jump to
S1C1
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -134.192692 |
| 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 HF/6-31G
Geometric Data calculated at HF/6-31G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability