Jump to
S1C2
Energy calculated at M06-2X/6-31G*
| | hartrees |
| Energy at 0K | -135.091446 |
| Energy at 298.15K | -135.099644 |
| HF Energy | -135.091446 |
| Nuclear repulsion energy | 82.809663 |
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 M06-2X/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' |
3496 |
3311 |
0.67 |
|
|
|
| 2 |
A' |
3149 |
2982 |
35.67 |
|
|
|
| 3 |
A' |
3092 |
2928 |
34.08 |
|
|
|
| 4 |
A' |
3071 |
2908 |
17.17 |
|
|
|
| 5 |
A' |
1703 |
1613 |
24.40 |
|
|
|
| 6 |
A' |
1537 |
1455 |
1.93 |
|
|
|
| 7 |
A' |
1519 |
1439 |
0.00 |
|
|
|
| 8 |
A' |
1442 |
1365 |
9.45 |
|
|
|
| 9 |
A' |
1401 |
1327 |
15.37 |
|
|
|
| 10 |
A' |
1182 |
1119 |
9.84 |
|
|
|
| 11 |
A' |
1101 |
1043 |
32.41 |
|
|
|
| 12 |
A' |
918 |
869 |
90.14 |
|
|
|
| 13 |
A' |
897 |
849 |
96.11 |
|
|
|
| 14 |
A' |
407 |
386 |
6.83 |
|
|
|
| 15 |
A" |
3582 |
3392 |
0.02 |
|
|
|
| 16 |
A" |
3155 |
2988 |
56.80 |
|
|
|
| 17 |
A" |
3127 |
2961 |
3.70 |
|
|
|
| 18 |
A" |
1530 |
1449 |
7.27 |
|
|
|
| 19 |
A" |
1409 |
1334 |
0.00 |
|
|
|
| 20 |
A" |
1288 |
1220 |
0.05 |
|
|
|
| 21 |
A" |
1018 |
964 |
1.76 |
|
|
|
| 22 |
A" |
783 |
741 |
0.85 |
|
|
|
| 23 |
A" |
314 |
298 |
48.89 |
|
|
|
| 24 |
A" |
258 |
244 |
9.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20689.0 cm
-1
Scaled (by 0.947) Zero Point Vibrational Energy (zpe) 19592.5 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 M06-2X/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.304 |
-0.083 |
0.000 |
| C2 |
0.000 |
0.577 |
0.000 |
| C3 |
1.208 |
-0.359 |
0.000 |
| H4 |
2.151 |
0.198 |
0.000 |
| H5 |
1.198 |
-1.005 |
0.885 |
| H6 |
1.198 |
-1.005 |
-0.885 |
| H7 |
0.039 |
1.234 |
-0.876 |
| H8 |
0.039 |
1.234 |
0.876 |
| H9 |
-1.372 |
-0.693 |
0.812 |
| H10 |
-1.372 |
-0.693 |
-0.812 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4617 | 2.5278 | 3.4666 | 2.8101 | 2.8101 | 2.0746 | 2.0746 | 1.0185 | 1.0185 |
C2 | 1.4617 | | 1.5285 | 2.1840 | 2.1729 | 2.1729 | 1.0955 | 1.0955 | 2.0389 | 2.0389 | C3 | 2.5278 | 1.5285 | | 1.0949 | 1.0958 | 1.0958 | 2.1615 | 2.1615 | 2.7261 | 2.7261 | H4 | 3.4666 | 2.1840 | 1.0949 | | 1.7714 | 1.7714 | 2.5102 | 2.5102 | 3.7240 | 3.7240 | H5 | 2.8101 | 2.1729 | 1.0958 | 1.7714 | | 1.7705 | 3.0752 | 2.5208 | 2.5905 | 3.0964 | H6 | 2.8101 | 2.1729 | 1.0958 | 1.7714 | 1.7705 | | 2.5208 | 3.0752 | 3.0964 | 2.5905 | H7 | 2.0746 | 1.0955 | 2.1615 | 2.5102 | 3.0752 | 2.5208 | | 1.7525 | 2.9249 | 2.3890 | H8 | 2.0746 | 1.0955 | 2.1615 | 2.5102 | 2.5208 | 3.0752 | 1.7525 | | 2.3890 | 2.9249 | H9 | 1.0185 | 2.0389 | 2.7261 | 3.7240 | 2.5905 | 3.0964 | 2.9249 | 2.3890 | | 1.6248 | H10 | 1.0185 | 2.0389 | 2.7261 | 3.7240 | 3.0964 | 2.5905 | 2.3890 | 2.9249 | 1.6248 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.402 |
|
N1 |
C2 |
H7 |
107.578 |
| N1 |
C2 |
H8 |
107.578 |
|
C2 |
N1 |
H9 |
109.279 |
| C2 |
N1 |
H10 |
109.279 |
|
C2 |
C3 |
H4 |
111.651 |
| C2 |
C3 |
H5 |
110.712 |
|
C2 |
C3 |
H6 |
110.712 |
| C3 |
C2 |
H7 |
109.819 |
|
C3 |
C2 |
H8 |
109.819 |
| H4 |
C3 |
H5 |
107.920 |
|
H4 |
C3 |
H6 |
107.920 |
| H5 |
C3 |
H6 |
107.779 |
|
H7 |
C2 |
H8 |
106.226 |
| H9 |
N1 |
H10 |
105.819 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.741 |
|
|
|
| 2 |
C |
-0.173 |
|
|
|
| 3 |
C |
-0.485 |
|
|
|
| 4 |
H |
0.159 |
|
|
|
| 5 |
H |
0.151 |
|
|
|
| 6 |
H |
0.151 |
|
|
|
| 7 |
H |
0.162 |
|
|
|
| 8 |
H |
0.162 |
|
|
|
| 9 |
H |
0.307 |
|
|
|
| 10 |
H |
0.307 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.043 |
-1.072 |
0.000 |
1.495 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.043 |
2.679 |
0.000 |
| y |
2.679 |
-20.071 |
0.000 |
| z |
0.000 |
0.000 |
-19.028 |
|
| Traceless |
| | x | y | z |
| x |
-4.494 |
2.679 |
0.000 |
| y |
2.679 |
1.465 |
0.000 |
| z |
0.000 |
0.000 |
3.029 |
|
| Polar |
| 3z2-r2 | 6.058 |
| x2-y2 | -3.972 |
| xy | 2.679 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.604 |
0.268 |
0.000 |
| y |
0.268 |
4.241 |
0.000 |
| z |
0.000 |
0.000 |
4.343 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at M06-2X/6-31G*
| | hartrees |
| Energy at 0K | -135.091013 |
| 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 M06-2X/6-31G*
Geometric Data calculated at M06-2X/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability