Jump to
S1C2
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -135.090811 |
| Energy at 298.15K | -135.098921 |
| Nuclear repulsion energy | 81.725993 |
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/cc-pVDZ
| 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' |
3310 |
3315 |
7.06 |
|
|
|
| 2 |
A' |
2998 |
3003 |
53.64 |
|
|
|
| 3 |
A' |
2937 |
2941 |
34.80 |
|
|
|
| 4 |
A' |
2930 |
2935 |
35.32 |
|
|
|
| 5 |
A' |
1607 |
1610 |
10.88 |
|
|
|
| 6 |
A' |
1438 |
1441 |
0.61 |
|
|
|
| 7 |
A' |
1417 |
1419 |
0.06 |
|
|
|
| 8 |
A' |
1351 |
1353 |
3.55 |
|
|
|
| 9 |
A' |
1328 |
1330 |
21.38 |
|
|
|
| 10 |
A' |
1118 |
1120 |
8.38 |
|
|
|
| 11 |
A' |
1019 |
1020 |
23.78 |
|
|
|
| 12 |
A' |
888 |
890 |
101.90 |
|
|
|
| 13 |
A' |
837 |
838 |
48.36 |
|
|
|
| 14 |
A' |
389 |
389 |
4.93 |
|
|
|
| 15 |
A" |
3380 |
3386 |
4.03 |
|
|
|
| 16 |
A" |
3004 |
3009 |
62.66 |
|
|
|
| 17 |
A" |
2965 |
2969 |
11.68 |
|
|
|
| 18 |
A" |
1426 |
1428 |
6.13 |
|
|
|
| 19 |
A" |
1349 |
1351 |
0.01 |
|
|
|
| 20 |
A" |
1228 |
1230 |
0.20 |
|
|
|
| 21 |
A" |
982 |
983 |
0.98 |
|
|
|
| 22 |
A" |
762 |
763 |
1.12 |
|
|
|
| 23 |
A" |
307 |
308 |
31.96 |
|
|
|
| 24 |
A" |
254 |
255 |
7.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19611.7 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 19643.1 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 BLYP/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.328 |
-0.074 |
0.000 |
| C2 |
0.000 |
0.578 |
0.000 |
| C3 |
1.224 |
-0.364 |
0.000 |
| H4 |
2.180 |
0.203 |
0.000 |
| H5 |
1.223 |
-1.021 |
0.897 |
| H6 |
1.223 |
-1.021 |
-0.897 |
| H7 |
0.046 |
1.246 |
-0.888 |
| H8 |
0.046 |
1.246 |
0.888 |
| H9 |
-1.384 |
-0.707 |
0.815 |
| H10 |
-1.384 |
-0.707 |
-0.815 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4793 | 2.5690 | 3.5195 | 2.8653 | 2.8653 | 2.1018 | 2.1018 | 1.0336 | 1.0336 |
C2 | 1.4793 | | 1.5449 | 2.2124 | 2.2038 | 2.2038 | 1.1122 | 1.1122 | 2.0570 | 2.0570 | C3 | 2.5690 | 1.5449 | | 1.1118 | 1.1117 | 1.1117 | 2.1843 | 2.1843 | 2.7544 | 2.7544 | H4 | 3.5195 | 2.2124 | 1.1118 | | 1.7946 | 1.7946 | 2.5364 | 2.5364 | 3.7683 | 3.7683 | H5 | 2.8653 | 2.2038 | 1.1117 | 1.7946 | | 1.7936 | 3.1164 | 2.5550 | 2.6273 | 3.1346 | H6 | 2.8653 | 2.2038 | 1.1117 | 1.7946 | 1.7936 | | 2.5550 | 3.1164 | 3.1346 | 2.6273 | H7 | 2.1018 | 1.1122 | 2.1843 | 2.5364 | 3.1164 | 2.5550 | | 1.7754 | 2.9596 | 2.4220 | H8 | 2.1018 | 1.1122 | 2.1843 | 2.5364 | 2.5550 | 3.1164 | 1.7754 | | 2.4220 | 2.9596 | H9 | 1.0336 | 2.0570 | 2.7544 | 3.7683 | 2.6273 | 3.1346 | 2.9596 | 2.4220 | | 1.6296 | H10 | 1.0336 | 2.0570 | 2.7544 | 3.7683 | 3.1346 | 2.6273 | 2.4220 | 2.9596 | 1.6296 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.296 |
|
N1 |
C2 |
H7 |
107.555 |
| N1 |
C2 |
H8 |
107.555 |
|
C2 |
N1 |
H9 |
108.585 |
| C2 |
N1 |
H10 |
108.585 |
|
C2 |
C3 |
H4 |
111.734 |
| C2 |
C3 |
H5 |
111.057 |
|
C2 |
C3 |
H6 |
111.057 |
| C3 |
C2 |
H7 |
109.509 |
|
C3 |
C2 |
H8 |
109.509 |
| H4 |
C3 |
H5 |
107.627 |
|
H4 |
C3 |
H6 |
107.627 |
| H5 |
C3 |
H6 |
107.547 |
|
H7 |
C2 |
H8 |
105.902 |
| H9 |
N1 |
H10 |
104.053 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.143 |
|
|
|
| 2 |
C |
0.026 |
|
|
|
| 3 |
C |
-0.001 |
|
|
|
| 4 |
H |
-0.002 |
|
|
|
| 5 |
H |
-0.000 |
|
|
|
| 6 |
H |
-0.000 |
|
|
|
| 7 |
H |
0.004 |
|
|
|
| 8 |
H |
0.004 |
|
|
|
| 9 |
H |
0.057 |
|
|
|
| 10 |
H |
0.057 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.719 |
-0.907 |
0.000 |
1.158 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.709 |
2.342 |
0.000 |
| y |
2.342 |
-20.425 |
0.000 |
| z |
0.000 |
0.000 |
-19.516 |
|
| Traceless |
| | x | y | z |
| x |
-3.739 |
2.342 |
0.000 |
| y |
2.342 |
1.188 |
0.000 |
| z |
0.000 |
0.000 |
2.551 |
|
| Polar |
| 3z2-r2 | 5.102 |
| x2-y2 | -3.285 |
| xy | 2.342 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.369 |
0.207 |
0.000 |
| y |
0.207 |
4.777 |
0.000 |
| z |
0.000 |
0.000 |
4.691 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -135.089728 |
| 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/cc-pVDZ
Geometric Data calculated at BLYP/cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability