Jump to
S1C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -135.122254 |
| Energy at 298.15K | -135.130430 |
| Nuclear repulsion energy | 82.684225 |
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 B3PW91/6-31G*
| 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' |
3479 |
3329 |
1.93 |
|
|
|
| 2 |
A' |
3120 |
2985 |
45.22 |
|
|
|
| 3 |
A' |
3056 |
2924 |
38.34 |
|
|
|
| 4 |
A' |
3042 |
2910 |
24.25 |
|
|
|
| 5 |
A' |
1703 |
1630 |
22.56 |
|
|
|
| 6 |
A' |
1529 |
1463 |
2.59 |
|
|
|
| 7 |
A' |
1511 |
1445 |
0.02 |
|
|
|
| 8 |
A' |
1432 |
1370 |
8.45 |
|
|
|
| 9 |
A' |
1396 |
1335 |
14.71 |
|
|
|
| 10 |
A' |
1173 |
1122 |
10.18 |
|
|
|
| 11 |
A' |
1083 |
1036 |
29.49 |
|
|
|
| 12 |
A' |
913 |
874 |
94.05 |
|
|
|
| 13 |
A' |
882 |
844 |
97.89 |
|
|
|
| 14 |
A' |
401 |
384 |
6.48 |
|
|
|
| 15 |
A" |
3568 |
3413 |
0.45 |
|
|
|
| 16 |
A" |
3123 |
2988 |
63.56 |
|
|
|
| 17 |
A" |
3091 |
2957 |
5.88 |
|
|
|
| 18 |
A" |
1521 |
1455 |
7.66 |
|
|
|
| 19 |
A" |
1409 |
1348 |
0.00 |
|
|
|
| 20 |
A" |
1284 |
1229 |
0.02 |
|
|
|
| 21 |
A" |
1018 |
973 |
1.50 |
|
|
|
| 22 |
A" |
782 |
748 |
1.62 |
|
|
|
| 23 |
A" |
308 |
295 |
47.63 |
|
|
|
| 24 |
A" |
258 |
247 |
10.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20541.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 19651.6 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 B3PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.309 |
-0.077 |
0.000 |
| C2 |
0.000 |
0.572 |
0.000 |
| C3 |
1.213 |
-0.361 |
0.000 |
| H4 |
2.155 |
0.201 |
0.000 |
| H5 |
1.211 |
-1.009 |
0.886 |
| H6 |
1.211 |
-1.009 |
-0.886 |
| H7 |
0.042 |
1.232 |
-0.876 |
| H8 |
0.042 |
1.232 |
0.876 |
| H9 |
-1.386 |
-0.686 |
0.812 |
| H10 |
-1.386 |
-0.686 |
-0.812 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4610 | 2.5378 | 3.4750 | 2.8296 | 2.8296 | 2.0749 | 2.0749 | 1.0185 | 1.0185 |
C2 | 1.4610 | | 1.5299 | 2.1863 | 2.1796 | 2.1796 | 1.0976 | 1.0976 | 2.0407 | 2.0407 | C3 | 2.5378 | 1.5299 | | 1.0973 | 1.0976 | 1.0976 | 2.1620 | 2.1620 | 2.7423 | 2.7423 | H4 | 3.4750 | 2.1863 | 1.0973 | | 1.7721 | 1.7721 | 2.5083 | 2.5083 | 3.7399 | 3.7399 | H5 | 2.8296 | 2.1796 | 1.0976 | 1.7721 | | 1.7721 | 3.0809 | 2.5272 | 2.6186 | 3.1201 | H6 | 2.8296 | 2.1796 | 1.0976 | 1.7721 | 1.7721 | | 2.5272 | 3.0809 | 3.1201 | 2.6186 | H7 | 2.0749 | 1.0976 | 2.1620 | 2.5083 | 3.0809 | 2.5272 | | 1.7522 | 2.9274 | 2.3924 | H8 | 2.0749 | 1.0976 | 2.1620 | 2.5083 | 2.5272 | 3.0809 | 1.7522 | | 2.3924 | 2.9274 | H9 | 1.0185 | 2.0407 | 2.7423 | 3.7399 | 2.6186 | 3.1201 | 2.9274 | 2.3924 | | 1.6242 | H10 | 1.0185 | 2.0407 | 2.7423 | 3.7399 | 3.1201 | 2.6186 | 2.3924 | 2.9274 | 1.6242 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.080 |
|
N1 |
C2 |
H7 |
107.531 |
| N1 |
C2 |
H8 |
107.531 |
|
C2 |
N1 |
H9 |
109.490 |
| C2 |
N1 |
H10 |
109.490 |
|
C2 |
C3 |
H4 |
111.584 |
| C2 |
C3 |
H5 |
111.031 |
|
C2 |
C3 |
H6 |
111.031 |
| C3 |
C2 |
H7 |
109.643 |
|
C3 |
C2 |
H8 |
109.643 |
| H4 |
C3 |
H5 |
107.680 |
|
H4 |
C3 |
H6 |
107.680 |
| H5 |
C3 |
H6 |
107.657 |
|
H7 |
C2 |
H8 |
105.913 |
| H9 |
N1 |
H10 |
105.761 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.731 |
|
|
-1.000 |
| 2 |
C |
-0.193 |
|
|
0.448 |
| 3 |
C |
-0.514 |
|
|
-0.430 |
| 4 |
H |
0.165 |
|
|
0.080 |
| 5 |
H |
0.160 |
|
|
0.100 |
| 6 |
H |
0.160 |
|
|
0.100 |
| 7 |
H |
0.169 |
|
|
-0.013 |
| 8 |
H |
0.169 |
|
|
-0.013 |
| 9 |
H |
0.307 |
|
|
0.364 |
| 10 |
H |
0.307 |
|
|
0.364 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.983 |
-1.086 |
0.000 |
1.465 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.933 |
-1.105 |
0.000 |
1.447 |
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> |
58.522 |
| (<r2>)1/2 |
7.650 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -135.121587 |
| 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 B3PW91/6-31G*
Geometric Data calculated at B3PW91/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability