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S1C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -134.289785 |
| Energy at 298.15K | -134.298125 |
| Nuclear repulsion energy | 83.197501 |
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' |
3713 |
3374 |
0.09 |
|
|
|
| 2 |
A' |
3212 |
2918 |
78.75 |
|
|
|
| 3 |
A' |
3173 |
2883 |
35.09 |
|
|
|
| 4 |
A' |
3146 |
2858 |
34.62 |
|
|
|
| 5 |
A' |
1800 |
1635 |
28.30 |
|
|
|
| 6 |
A' |
1627 |
1478 |
1.38 |
|
|
|
| 7 |
A' |
1605 |
1458 |
0.46 |
|
|
|
| 8 |
A' |
1536 |
1395 |
14.17 |
|
|
|
| 9 |
A' |
1499 |
1362 |
13.44 |
|
|
|
| 10 |
A' |
1235 |
1122 |
12.66 |
|
|
|
| 11 |
A' |
1147 |
1042 |
45.27 |
|
|
|
| 12 |
A' |
959 |
872 |
84.07 |
|
|
|
| 13 |
A' |
931 |
846 |
97.42 |
|
|
|
| 14 |
A' |
430 |
391 |
6.59 |
|
|
|
| 15 |
A" |
3789 |
3442 |
0.10 |
|
|
|
| 16 |
A" |
3220 |
2925 |
109.76 |
|
|
|
| 17 |
A" |
3190 |
2898 |
0.14 |
|
|
|
| 18 |
A" |
1608 |
1461 |
6.49 |
|
|
|
| 19 |
A" |
1503 |
1365 |
0.08 |
|
|
|
| 20 |
A" |
1374 |
1248 |
0.07 |
|
|
|
| 21 |
A" |
1080 |
981 |
1.02 |
|
|
|
| 22 |
A" |
835 |
758 |
0.25 |
|
|
|
| 23 |
A" |
317 |
288 |
35.40 |
|
|
|
| 24 |
A" |
266 |
242 |
16.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21596.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 19620.5 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 HF/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.299 |
-0.082 |
0.000 |
| C2 |
0.000 |
0.574 |
0.000 |
| C3 |
1.209 |
-0.362 |
0.000 |
| H4 |
2.140 |
0.200 |
0.000 |
| H5 |
1.204 |
-1.002 |
0.879 |
| H6 |
1.204 |
-1.002 |
-0.879 |
| H7 |
0.043 |
1.224 |
-0.869 |
| H8 |
0.043 |
1.224 |
0.869 |
| H9 |
-1.398 |
-0.670 |
0.804 |
| H10 |
-1.398 |
-0.670 |
-0.804 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4548 | 2.5227 | 3.4499 | 2.8076 | 2.8076 | 2.0645 | 2.0645 | 1.0009 | 1.0009 |
C2 | 1.4548 | | 1.5282 | 2.1722 | 2.1693 | 2.1693 | 1.0862 | 1.0862 | 2.0366 | 2.0366 | C3 | 2.5227 | 1.5282 | | 1.0873 | 1.0876 | 1.0876 | 2.1509 | 2.1509 | 2.7455 | 2.7455 | H4 | 3.4499 | 2.1722 | 1.0873 | | 1.7585 | 1.7585 | 2.4897 | 2.4897 | 3.7310 | 3.7310 | H5 | 2.8076 | 2.1693 | 1.0876 | 1.7585 | | 1.7578 | 3.0591 | 2.5106 | 2.6247 | 3.1172 | H6 | 2.8076 | 2.1693 | 1.0876 | 1.7585 | 1.7578 | | 2.5106 | 3.0591 | 3.1172 | 2.6247 | H7 | 2.0645 | 1.0862 | 2.1509 | 2.4897 | 3.0591 | 2.5106 | | 1.7379 | 2.9092 | 2.3808 | H8 | 2.0645 | 1.0862 | 2.1509 | 2.4897 | 2.5106 | 3.0591 | 1.7379 | | 2.3808 | 2.9092 | H9 | 1.0009 | 2.0366 | 2.7455 | 3.7310 | 2.6247 | 3.1172 | 2.9092 | 2.3808 | | 1.6086 | H10 | 1.0009 | 2.0366 | 2.7455 | 3.7310 | 3.1172 | 2.6247 | 2.3808 | 2.9092 | 1.6086 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.471 |
|
N1 |
C2 |
H7 |
107.795 |
| N1 |
C2 |
H8 |
107.795 |
|
C2 |
N1 |
H9 |
110.700 |
| C2 |
N1 |
H10 |
110.700 |
|
C2 |
C3 |
H4 |
111.189 |
| C2 |
C3 |
H5 |
110.932 |
|
C2 |
C3 |
H6 |
110.932 |
| C3 |
C2 |
H7 |
109.556 |
|
C3 |
C2 |
H8 |
109.556 |
| H4 |
C3 |
H5 |
107.910 |
|
H4 |
C3 |
H6 |
107.910 |
| H5 |
C3 |
H6 |
107.824 |
|
H7 |
C2 |
H8 |
106.259 |
| H9 |
N1 |
H10 |
106.944 |
|
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 |
N |
-0.494 |
|
|
|
| 2 |
C |
-0.036 |
|
|
|
| 3 |
C |
-0.245 |
|
|
|
| 4 |
H |
0.085 |
|
|
|
| 5 |
H |
0.076 |
|
|
|
| 6 |
H |
0.076 |
|
|
|
| 7 |
H |
0.090 |
|
|
|
| 8 |
H |
0.090 |
|
|
|
| 9 |
H |
0.178 |
|
|
|
| 10 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.946 |
-0.966 |
0.000 |
1.352 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.048 |
2.704 |
0.000 |
| y |
2.704 |
-20.378 |
0.000 |
| z |
0.000 |
0.000 |
-19.119 |
|
| Traceless |
| | x | y | z |
| x |
-4.300 |
2.704 |
0.000 |
| y |
2.704 |
1.206 |
0.000 |
| z |
0.000 |
0.000 |
3.094 |
|
| Polar |
| 3z2-r2 | 6.188 |
| x2-y2 | -3.670 |
| xy | 2.704 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.776 |
0.151 |
0.000 |
| y |
0.151 |
4.427 |
0.000 |
| z |
0.000 |
0.000 |
4.414 |
<r2> (average value of r
2) Å
2
| <r2> |
58.287 |
| (<r2>)1/2 |
7.635 |
Jump to
S1C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -134.289815 |
| 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/6-311G**
Geometric Data calculated at HF/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability