Jump to
S1C2
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -133.490019 |
| Energy at 298.15K | -133.498017 |
| Nuclear repulsion energy | 80.926176 |
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/STO-3G
| 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' |
3474 |
3100 |
2.70 |
|
|
|
| 2 |
A' |
3462 |
3089 |
17.32 |
|
|
|
| 3 |
A' |
3331 |
2973 |
4.99 |
|
|
|
| 4 |
A' |
3303 |
2947 |
1.71 |
|
|
|
| 5 |
A' |
1866 |
1665 |
4.48 |
|
|
|
| 6 |
A' |
1691 |
1509 |
1.39 |
|
|
|
| 7 |
A' |
1652 |
1474 |
0.13 |
|
|
|
| 8 |
A' |
1571 |
1402 |
1.19 |
|
|
|
| 9 |
A' |
1483 |
1324 |
13.16 |
|
|
|
| 10 |
A' |
1267 |
1131 |
11.71 |
|
|
|
| 11 |
A' |
1119 |
998 |
2.80 |
|
|
|
| 12 |
A' |
1033 |
922 |
64.67 |
|
|
|
| 13 |
A' |
924 |
825 |
14.64 |
|
|
|
| 14 |
A' |
399 |
356 |
5.54 |
|
|
|
| 15 |
A" |
3646 |
3254 |
18.96 |
|
|
|
| 16 |
A" |
3475 |
3101 |
3.55 |
|
|
|
| 17 |
A" |
3437 |
3067 |
0.80 |
|
|
|
| 18 |
A" |
1686 |
1504 |
4.90 |
|
|
|
| 19 |
A" |
1512 |
1350 |
0.62 |
|
|
|
| 20 |
A" |
1381 |
1233 |
0.01 |
|
|
|
| 21 |
A" |
1090 |
973 |
3.85 |
|
|
|
| 22 |
A" |
836 |
746 |
2.36 |
|
|
|
| 23 |
A" |
317 |
283 |
50.03 |
|
|
|
| 24 |
A" |
224 |
200 |
2.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 22090.0 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 19713.1 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.357 |
-0.088 |
0.000 |
| C2 |
0.000 |
0.597 |
0.000 |
| C3 |
1.236 |
-0.360 |
0.000 |
| H4 |
2.171 |
0.221 |
0.000 |
| H5 |
1.230 |
-1.004 |
0.893 |
| H6 |
1.230 |
-1.004 |
-0.893 |
| H7 |
0.041 |
1.249 |
-0.893 |
| H8 |
0.041 |
1.249 |
0.893 |
| H9 |
-1.316 |
-0.759 |
0.824 |
| H10 |
-1.316 |
-0.759 |
-0.824 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.5203 | 2.6072 | 3.5418 | 2.8854 | 2.8854 | 2.1305 | 2.1305 | 1.0633 | 1.0633 |
C2 | 1.5203 | | 1.5634 | 2.2037 | 2.2077 | 2.2077 | 1.1063 | 1.1063 | 2.0617 | 2.0617 | C3 | 2.6072 | 1.5634 | | 1.1010 | 1.1014 | 1.1014 | 2.1942 | 2.1942 | 2.7114 | 2.7114 | H4 | 3.5418 | 2.2037 | 1.1010 | | 1.7851 | 1.7851 | 2.5285 | 2.5285 | 3.7150 | 3.7150 | H5 | 2.8854 | 2.2077 | 1.1014 | 1.7851 | | 1.7866 | 3.1112 | 2.5473 | 2.5581 | 3.0802 | H6 | 2.8854 | 2.2077 | 1.1014 | 1.7851 | 1.7866 | | 2.5473 | 3.1112 | 3.0802 | 2.5581 | H7 | 2.1305 | 1.1063 | 2.1942 | 2.5285 | 3.1112 | 2.5473 | | 1.7863 | 2.9700 | 2.4244 | H8 | 2.1305 | 1.1063 | 2.1942 | 2.5285 | 2.5473 | 3.1112 | 1.7863 | | 2.4244 | 2.9700 | H9 | 1.0633 | 2.0617 | 2.7114 | 3.7150 | 2.5581 | 3.0802 | 2.9700 | 2.4244 | | 1.6478 | H10 | 1.0633 | 2.0617 | 2.7114 | 3.7150 | 3.0802 | 2.5581 | 2.4244 | 2.9700 | 1.6478 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.443 |
|
N1 |
C2 |
H7 |
107.366 |
| N1 |
C2 |
H8 |
107.366 |
|
C2 |
N1 |
H9 |
104.489 |
| C2 |
N1 |
H10 |
104.489 |
|
C2 |
C3 |
H4 |
110.395 |
| C2 |
C3 |
H5 |
110.687 |
|
C2 |
C3 |
H6 |
110.687 |
| C3 |
C2 |
H7 |
109.357 |
|
C3 |
C2 |
H8 |
109.357 |
| H4 |
C3 |
H5 |
108.293 |
|
H4 |
C3 |
H6 |
108.293 |
| H5 |
C3 |
H6 |
108.404 |
|
H7 |
C2 |
H8 |
107.671 |
| H9 |
N1 |
H10 |
101.587 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.362 |
|
|
|
| 2 |
C |
-0.068 |
|
|
|
| 3 |
C |
-0.228 |
|
|
|
| 4 |
H |
0.077 |
|
|
|
| 5 |
H |
0.070 |
|
|
|
| 6 |
H |
0.070 |
|
|
|
| 7 |
H |
0.076 |
|
|
|
| 8 |
H |
0.076 |
|
|
|
| 9 |
H |
0.145 |
|
|
|
| 10 |
H |
0.145 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.314 |
-1.080 |
0.000 |
1.701 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.805 |
2.086 |
0.000 |
| y |
2.086 |
-18.426 |
0.000 |
| z |
0.000 |
0.000 |
-18.137 |
|
| Traceless |
| | x | y | z |
| x |
-4.524 |
2.086 |
0.000 |
| y |
2.086 |
2.045 |
0.000 |
| z |
0.000 |
0.000 |
2.479 |
|
| Polar |
| 3z2-r2 | 4.958 |
| x2-y2 | -4.379 |
| xy | 2.086 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.349 |
0.314 |
0.000 |
| y |
0.314 |
2.247 |
0.000 |
| z |
0.000 |
0.000 |
2.389 |
<r2> (average value of r
2) Å
2
| <r2> |
59.480 |
| (<r2>)1/2 |
7.712 |
Jump to
S1C1
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -133.488529 |
| 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 B3LYP/STO-3G
Geometric Data calculated at B3LYP/STO-3G
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability