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S1C2
Energy calculated at G4
| | hartrees |
| Energy at 0K | -135.058694 |
| Energy at 298.15K | -135.053328 |
| HF Energy | -135.186629 |
| Nuclear repulsion energy | 82.591465 |
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 B3LYP/6-31G(2df,p)
| 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' |
3473 |
3352 |
1.12 |
|
|
|
| 2 |
A' |
3091 |
2983 |
43.88 |
|
|
|
| 3 |
A' |
3026 |
2920 |
37.68 |
|
|
|
| 4 |
A' |
3019 |
2913 |
21.16 |
|
|
|
| 5 |
A' |
1666 |
1608 |
16.87 |
|
|
|
| 6 |
A' |
1506 |
1453 |
0.92 |
|
|
|
| 7 |
A' |
1485 |
1433 |
0.01 |
|
|
|
| 8 |
A' |
1407 |
1358 |
4.86 |
|
|
|
| 9 |
A' |
1383 |
1335 |
16.21 |
|
|
|
| 10 |
A' |
1157 |
1116 |
9.74 |
|
|
|
| 11 |
A' |
1061 |
1024 |
24.82 |
|
|
|
| 12 |
A' |
907 |
875 |
83.09 |
|
|
|
| 13 |
A' |
864 |
834 |
79.05 |
|
|
|
| 14 |
A' |
400 |
386 |
5.20 |
|
|
|
| 15 |
A" |
3548 |
3424 |
0.14 |
|
|
|
| 16 |
A" |
3093 |
2985 |
56.60 |
|
|
|
| 17 |
A" |
3055 |
2948 |
8.50 |
|
|
|
| 18 |
A" |
1495 |
1443 |
5.36 |
|
|
|
| 19 |
A" |
1395 |
1346 |
0.03 |
|
|
|
| 20 |
A" |
1273 |
1229 |
0.04 |
|
|
|
| 21 |
A" |
1009 |
974 |
1.05 |
|
|
|
| 22 |
A" |
778 |
751 |
1.08 |
|
|
|
| 23 |
A" |
295 |
285 |
32.67 |
|
|
|
| 24 |
A" |
254 |
245 |
11.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20320.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 19609.0 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 B3LYP/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.312 |
-0.079 |
0.000 |
| C2 |
0.000 |
0.574 |
0.000 |
| C3 |
1.215 |
-0.361 |
0.000 |
| H4 |
2.155 |
0.202 |
0.000 |
| H5 |
1.212 |
-1.008 |
0.885 |
| H6 |
1.212 |
-1.008 |
-0.885 |
| H7 |
0.044 |
1.233 |
-0.876 |
| H8 |
0.044 |
1.233 |
0.876 |
| H9 |
-1.387 |
-0.690 |
0.810 |
| H10 |
-1.387 |
-0.690 |
-0.810 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4655 | 2.5427 | 3.4785 | 2.8313 | 2.8313 | 2.0803 | 2.0803 | 1.0170 | 1.0170 |
C2 | 1.4655 | | 1.5335 | 2.1871 | 2.1808 | 2.1808 | 1.0971 | 1.0971 | 2.0435 | 2.0435 | C3 | 2.5427 | 1.5335 | | 1.0961 | 1.0964 | 1.0964 | 2.1634 | 2.1634 | 2.7445 | 2.7445 | H4 | 3.4785 | 2.1871 | 1.0961 | | 1.7717 | 1.7717 | 2.5073 | 2.5073 | 3.7411 | 3.7411 | H5 | 2.8313 | 2.1808 | 1.0964 | 1.7717 | | 1.7704 | 3.0803 | 2.5271 | 2.6189 | 3.1186 | H6 | 2.8313 | 2.1808 | 1.0964 | 1.7717 | 1.7704 | | 2.5271 | 3.0803 | 3.1186 | 2.6189 | H7 | 2.0803 | 1.0971 | 2.1634 | 2.5073 | 3.0803 | 2.5271 | | 1.7523 | 2.9302 | 2.3976 | H8 | 2.0803 | 1.0971 | 2.1634 | 2.5073 | 2.5271 | 3.0803 | 1.7523 | | 2.3976 | 2.9302 | H9 | 1.0170 | 2.0435 | 2.7445 | 3.7411 | 2.6189 | 3.1186 | 2.9302 | 2.3976 | | 1.6195 | H10 | 1.0170 | 2.0435 | 2.7445 | 3.7411 | 3.1186 | 2.6189 | 2.3976 | 2.9302 | 1.6195 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.987 |
|
N1 |
C2 |
H7 |
107.760 |
| N1 |
C2 |
H8 |
107.760 |
|
C2 |
N1 |
H9 |
110.219 |
| C2 |
N1 |
H10 |
110.219 |
|
C2 |
C3 |
H4 |
111.566 |
| C2 |
C3 |
H5 |
110.877 |
|
C2 |
C3 |
H6 |
110.877 |
| C3 |
C2 |
H7 |
109.423 |
|
C3 |
C2 |
H8 |
109.423 |
| H4 |
C3 |
H5 |
107.819 |
|
H4 |
C3 |
H6 |
107.819 |
| H5 |
C3 |
H6 |
107.721 |
|
H7 |
C2 |
H8 |
106.018 |
| H9 |
N1 |
H10 |
106.467 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.494 |
|
|
|
| 2 |
C |
-0.115 |
|
|
|
| 3 |
C |
-0.368 |
|
|
|
| 4 |
H |
0.111 |
|
|
|
| 5 |
H |
0.108 |
|
|
|
| 6 |
H |
0.108 |
|
|
|
| 7 |
H |
0.105 |
|
|
|
| 8 |
H |
0.105 |
|
|
|
| 9 |
H |
0.220 |
|
|
|
| 10 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.838 |
-0.936 |
0.000 |
1.256 |
| CHELPG |
|
|
|
|
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
58.646 |
| (<r2>)1/2 |
7.658 |
Jump to
S1C1
Energy calculated at G4
| | hartrees |
| Energy at 0K | -135.058911 |
| Energy at 298.15K | -135.053517 |
| 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 B3LYP/6-31G(2df,p)
Geometric Data calculated at B3LYP/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability