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S1C2
Energy calculated at B3LYP/Def2TZVPP
| | hartrees |
| Energy at 0K | -135.236585 |
| Energy at 298.15K | -135.244707 |
| HF Energy | -135.236585 |
| Nuclear repulsion energy | 82.754808 |
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/Def2TZVPP
| 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' |
3484 |
3354 |
1.15 |
|
|
|
| 2 |
A' |
3079 |
2964 |
48.90 |
|
|
|
| 3 |
A' |
3028 |
2915 |
33.48 |
|
|
|
| 4 |
A' |
3016 |
2903 |
23.72 |
|
|
|
| 5 |
A' |
1661 |
1599 |
20.57 |
|
|
|
| 6 |
A' |
1506 |
1450 |
2.38 |
|
|
|
| 7 |
A' |
1488 |
1432 |
0.23 |
|
|
|
| 8 |
A' |
1410 |
1357 |
6.74 |
|
|
|
| 9 |
A' |
1385 |
1333 |
12.86 |
|
|
|
| 10 |
A' |
1145 |
1102 |
9.26 |
|
|
|
| 11 |
A' |
1057 |
1018 |
26.80 |
|
|
|
| 12 |
A' |
892 |
858 |
33.45 |
|
|
|
| 13 |
A' |
841 |
809 |
143.57 |
|
|
|
| 14 |
A' |
403 |
387 |
6.32 |
|
|
|
| 15 |
A" |
3560 |
3427 |
0.15 |
|
|
|
| 16 |
A" |
3086 |
2970 |
60.56 |
|
|
|
| 17 |
A" |
3052 |
2938 |
4.77 |
|
|
|
| 18 |
A" |
1494 |
1438 |
7.33 |
|
|
|
| 19 |
A" |
1389 |
1337 |
0.06 |
|
|
|
| 20 |
A" |
1272 |
1224 |
0.05 |
|
|
|
| 21 |
A" |
1008 |
970 |
0.76 |
|
|
|
| 22 |
A" |
781 |
752 |
1.05 |
|
|
|
| 23 |
A" |
280 |
270 |
28.54 |
|
|
|
| 24 |
A" |
249 |
240 |
16.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20280.8 cm
-1
Scaled (by 0.9626) Zero Point Vibrational Energy (zpe) 19522.3 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/Def2TZVPP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.309 |
-0.096 |
0.000 |
| C2 |
0.000 |
0.571 |
0.000 |
| C3 |
1.218 |
-0.346 |
0.000 |
| H4 |
2.152 |
0.222 |
0.000 |
| H5 |
1.225 |
-0.992 |
0.882 |
| H6 |
1.225 |
-0.992 |
-0.882 |
| H7 |
0.032 |
1.229 |
-0.872 |
| H8 |
0.032 |
1.229 |
0.872 |
| H9 |
-1.406 |
-0.687 |
0.816 |
| H10 |
-1.406 |
-0.687 |
-0.816 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4687 | 2.5385 | 3.4754 | 2.8280 | 2.8280 | 2.0768 | 2.0768 | 1.0120 | 1.0120 |
C2 | 1.4687 | | 1.5244 | 2.1803 | 2.1724 | 2.1724 | 1.0928 | 1.0928 | 2.0555 | 2.0555 | C3 | 2.5385 | 1.5244 | | 1.0941 | 1.0927 | 1.0927 | 2.1554 | 2.1554 | 2.7688 | 2.7688 | H4 | 3.4754 | 2.1803 | 1.0941 | | 1.7640 | 1.7640 | 2.5034 | 2.5034 | 3.7624 | 3.7624 | H5 | 2.8280 | 2.1724 | 1.0927 | 1.7640 | | 1.7632 | 3.0705 | 2.5206 | 2.6495 | 3.1459 | H6 | 2.8280 | 2.1724 | 1.0927 | 1.7640 | 1.7632 | | 2.5206 | 3.0705 | 3.1459 | 2.6495 | H7 | 2.0768 | 1.0928 | 2.1554 | 2.5034 | 3.0705 | 2.5206 | | 1.7437 | 2.9305 | 2.3965 | H8 | 2.0768 | 1.0928 | 2.1554 | 2.5034 | 2.5206 | 3.0705 | 1.7437 | | 2.3965 | 2.9305 | H9 | 1.0120 | 2.0555 | 2.7688 | 3.7624 | 2.6495 | 3.1459 | 2.9305 | 2.3965 | | 1.6314 | H10 | 1.0120 | 2.0555 | 2.7688 | 3.7624 | 3.1459 | 2.6495 | 2.3965 | 2.9305 | 1.6314 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.009 |
|
N1 |
C2 |
H7 |
107.444 |
| N1 |
C2 |
H8 |
107.444 |
|
C2 |
N1 |
H9 |
110.561 |
| C2 |
N1 |
H10 |
110.561 |
|
C2 |
C3 |
H4 |
111.697 |
| C2 |
C3 |
H5 |
111.144 |
|
C2 |
C3 |
H6 |
111.144 |
| C3 |
C2 |
H7 |
109.792 |
|
C3 |
C2 |
H8 |
109.792 |
| H4 |
C3 |
H5 |
107.543 |
|
H4 |
C3 |
H6 |
107.543 |
| H5 |
C3 |
H6 |
107.568 |
|
H7 |
C2 |
H8 |
105.853 |
| H9 |
N1 |
H10 |
107.417 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.329 |
|
|
|
| 2 |
C |
-0.008 |
|
|
|
| 3 |
C |
-0.232 |
|
|
|
| 4 |
H |
0.068 |
|
|
|
| 5 |
H |
0.066 |
|
|
|
| 6 |
H |
0.066 |
|
|
|
| 7 |
H |
0.069 |
|
|
|
| 8 |
H |
0.069 |
|
|
|
| 9 |
H |
0.116 |
|
|
|
| 10 |
H |
0.116 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.887 |
-0.893 |
0.000 |
1.258 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.174 |
2.568 |
0.000 |
| y |
2.568 |
-20.700 |
0.000 |
| z |
0.000 |
0.000 |
-19.367 |
|
| Traceless |
| | x | y | z |
| x |
-4.141 |
2.568 |
0.000 |
| y |
2.568 |
1.071 |
0.000 |
| z |
0.000 |
0.000 |
3.070 |
|
| Polar |
| 3z2-r2 | 6.140 |
| x2-y2 | -3.475 |
| xy | 2.568 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.862 |
0.072 |
0.000 |
| y |
0.072 |
5.209 |
0.000 |
| z |
0.000 |
0.000 |
4.997 |
<r2> (average value of r
2) Å
2
| <r2> |
58.913 |
| (<r2>)1/2 |
7.675 |
Jump to
S1C1
Energy calculated at B3LYP/Def2TZVPP
| | hartrees |
| Energy at 0K | -135.236475 |
| 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/Def2TZVPP
Geometric Data calculated at B3LYP/Def2TZVPP
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability