Jump to
S1C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -135.136489 |
| Energy at 298.15K | -135.144573 |
| Nuclear repulsion energy | 81.911401 |
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 BLYP/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' |
3356 |
3343 |
5.11 |
|
|
|
| 2 |
A' |
2995 |
2983 |
61.12 |
|
|
|
| 3 |
A' |
2947 |
2935 |
36.22 |
|
|
|
| 4 |
A' |
2936 |
2924 |
30.60 |
|
|
|
| 5 |
A' |
1625 |
1618 |
19.20 |
|
|
|
| 6 |
A' |
1470 |
1464 |
2.32 |
|
|
|
| 7 |
A' |
1451 |
1445 |
0.15 |
|
|
|
| 8 |
A' |
1370 |
1365 |
4.96 |
|
|
|
| 9 |
A' |
1343 |
1337 |
14.72 |
|
|
|
| 10 |
A' |
1114 |
1109 |
9.39 |
|
|
|
| 11 |
A' |
1005 |
1001 |
19.51 |
|
|
|
| 12 |
A' |
875 |
871 |
101.52 |
|
|
|
| 13 |
A' |
820 |
817 |
86.26 |
|
|
|
| 14 |
A' |
389 |
387 |
6.03 |
|
|
|
| 15 |
A" |
3428 |
3415 |
2.18 |
|
|
|
| 16 |
A" |
3004 |
2992 |
73.72 |
|
|
|
| 17 |
A" |
2969 |
2957 |
6.53 |
|
|
|
| 18 |
A" |
1460 |
1454 |
8.03 |
|
|
|
| 19 |
A" |
1357 |
1352 |
0.01 |
|
|
|
| 20 |
A" |
1239 |
1234 |
0.17 |
|
|
|
| 21 |
A" |
986 |
983 |
0.84 |
|
|
|
| 22 |
A" |
764 |
761 |
0.86 |
|
|
|
| 23 |
A" |
296 |
294 |
35.77 |
|
|
|
| 24 |
A" |
246 |
245 |
8.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19720.1 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 19643.2 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.326 |
-0.082 |
0.000 |
| C2 |
0.000 |
0.577 |
0.000 |
| C3 |
1.229 |
-0.360 |
0.000 |
| H4 |
2.173 |
0.209 |
0.000 |
| H5 |
1.228 |
-1.010 |
0.889 |
| H6 |
1.228 |
-1.010 |
-0.889 |
| H7 |
0.040 |
1.239 |
-0.880 |
| H8 |
0.040 |
1.239 |
0.880 |
| H9 |
-1.402 |
-0.697 |
0.817 |
| H10 |
-1.402 |
-0.697 |
-0.817 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4810 | 2.5705 | 3.5113 | 2.8595 | 2.8595 | 2.0942 | 2.0942 | 1.0253 | 1.0253 |
C2 | 1.4810 | | 1.5462 | 2.2043 | 2.1955 | 2.1955 | 1.1017 | 1.1017 | 2.0631 | 2.0631 | C3 | 2.5705 | 1.5462 | | 1.1021 | 1.1016 | 1.1016 | 2.1784 | 2.1784 | 2.7756 | 2.7756 | H4 | 3.5113 | 2.2043 | 1.1021 | | 1.7804 | 1.7804 | 2.5269 | 2.5269 | 3.7774 | 3.7774 | H5 | 2.8595 | 2.1955 | 1.1016 | 1.7804 | | 1.7789 | 3.0985 | 2.5433 | 2.6497 | 3.1508 | H6 | 2.8595 | 2.1955 | 1.1016 | 1.7804 | 1.7789 | | 2.5433 | 3.0985 | 3.1508 | 2.6497 | H7 | 2.0942 | 1.1017 | 2.1784 | 2.5269 | 3.0985 | 2.5433 | | 1.7607 | 2.9507 | 2.4144 | H8 | 2.0942 | 1.1017 | 2.1784 | 2.5269 | 2.5433 | 3.0985 | 1.7607 | | 2.4144 | 2.9507 | H9 | 1.0253 | 2.0631 | 2.7756 | 3.7774 | 2.6497 | 3.1508 | 2.9507 | 2.4144 | | 1.6340 | H10 | 1.0253 | 2.0631 | 2.7756 | 3.7774 | 3.1508 | 2.6497 | 2.4144 | 2.9507 | 1.6340 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.220 |
|
N1 |
C2 |
H7 |
107.453 |
| N1 |
C2 |
H8 |
107.453 |
|
C2 |
N1 |
H9 |
109.467 |
| C2 |
N1 |
H10 |
109.467 |
|
C2 |
C3 |
H4 |
111.577 |
| C2 |
C3 |
H5 |
110.914 |
|
C2 |
C3 |
H6 |
110.914 |
| C3 |
C2 |
H7 |
109.567 |
|
C3 |
C2 |
H8 |
109.567 |
| H4 |
C3 |
H5 |
107.789 |
|
H4 |
C3 |
H6 |
107.789 |
| H5 |
C3 |
H6 |
107.692 |
|
H7 |
C2 |
H8 |
106.091 |
| H9 |
N1 |
H10 |
105.657 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.422 |
|
|
|
| 2 |
C |
-0.131 |
|
|
|
| 3 |
C |
-0.291 |
|
|
|
| 4 |
H |
0.094 |
|
|
|
| 5 |
H |
0.089 |
|
|
|
| 6 |
H |
0.089 |
|
|
|
| 7 |
H |
0.109 |
|
|
|
| 8 |
H |
0.109 |
|
|
|
| 9 |
H |
0.176 |
|
|
|
| 10 |
H |
0.176 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.826 |
-0.913 |
0.000 |
1.231 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.261 |
2.588 |
0.000 |
| y |
2.588 |
-20.723 |
0.000 |
| z |
0.000 |
0.000 |
-19.581 |
|
| Traceless |
| | x | y | z |
| x |
-4.109 |
2.588 |
0.000 |
| y |
2.588 |
1.198 |
0.000 |
| z |
0.000 |
0.000 |
2.910 |
|
| Polar |
| 3z2-r2 | 5.821 |
| x2-y2 | -3.538 |
| xy | 2.588 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.634 |
0.142 |
0.000 |
| y |
0.142 |
4.954 |
0.000 |
| z |
0.000 |
0.000 |
4.847 |
<r2> (average value of r
2) Å
2
| <r2> |
59.911 |
| (<r2>)1/2 |
7.740 |
Jump to
S1C1
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -135.135669 |
| 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 BLYP/6-311G**
Geometric Data calculated at BLYP/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability