Jump to
S1C2
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -134.993024 |
| Energy at 298.15K | -135.001240 |
| HF Energy | -134.852497 |
| Nuclear repulsion energy | 82.692819 |
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 B2PLYP/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' |
3484 |
3307 |
1.74 |
|
|
|
| 2 |
A' |
3144 |
2984 |
45.26 |
|
|
|
| 3 |
A' |
3087 |
2930 |
35.47 |
|
|
|
| 4 |
A' |
3067 |
2911 |
21.98 |
|
|
|
| 5 |
A' |
1720 |
1633 |
21.91 |
|
|
|
| 6 |
A' |
1556 |
1477 |
1.70 |
|
|
|
| 7 |
A' |
1537 |
1459 |
0.00 |
|
|
|
| 8 |
A' |
1457 |
1383 |
6.10 |
|
|
|
| 9 |
A' |
1416 |
1344 |
16.95 |
|
|
|
| 10 |
A' |
1185 |
1124 |
11.76 |
|
|
|
| 11 |
A' |
1091 |
1036 |
27.73 |
|
|
|
| 12 |
A' |
932 |
885 |
120.85 |
|
|
|
| 13 |
A' |
892 |
846 |
63.38 |
|
|
|
| 14 |
A' |
407 |
386 |
6.60 |
|
|
|
| 15 |
A" |
3572 |
3391 |
0.64 |
|
|
|
| 16 |
A" |
3148 |
2988 |
67.91 |
|
|
|
| 17 |
A" |
3121 |
2962 |
2.12 |
|
|
|
| 18 |
A" |
1546 |
1468 |
6.49 |
|
|
|
| 19 |
A" |
1423 |
1351 |
0.00 |
|
|
|
| 20 |
A" |
1305 |
1239 |
0.05 |
|
|
|
| 21 |
A" |
1029 |
977 |
1.46 |
|
|
|
| 22 |
A" |
793 |
753 |
0.87 |
|
|
|
| 23 |
A" |
312 |
296 |
46.55 |
|
|
|
| 24 |
A" |
265 |
251 |
11.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20743.7 cm
-1
Scaled (by 0.9492) Zero Point Vibrational Energy (zpe) 19689.9 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 B2PLYP/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.310 |
-0.088 |
0.000 |
| C2 |
0.000 |
0.573 |
0.000 |
| C3 |
1.215 |
-0.353 |
0.000 |
| H4 |
2.156 |
0.210 |
0.000 |
| H5 |
1.215 |
-0.999 |
0.884 |
| H6 |
1.215 |
-0.999 |
-0.884 |
| H7 |
0.034 |
1.230 |
-0.874 |
| H8 |
0.034 |
1.230 |
0.874 |
| H9 |
-1.387 |
-0.689 |
0.815 |
| H10 |
-1.387 |
-0.689 |
-0.815 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4671 | 2.5389 | 3.4790 | 2.8266 | 2.8266 | 2.0753 | 2.0753 | 1.0159 | 1.0159 |
C2 | 1.4671 | | 1.5271 | 2.1865 | 2.1748 | 2.1748 | 1.0946 | 1.0946 | 2.0444 | 2.0444 | C3 | 2.5389 | 1.5271 | | 1.0964 | 1.0952 | 1.0952 | 2.1599 | 2.1599 | 2.7473 | 2.7473 | H4 | 3.4790 | 2.1865 | 1.0964 | | 1.7687 | 1.7687 | 2.5123 | 2.5123 | 3.7451 | 3.7451 | H5 | 2.8266 | 2.1748 | 1.0952 | 1.7687 | | 1.7676 | 3.0756 | 2.5234 | 2.6216 | 3.1233 | H6 | 2.8266 | 2.1748 | 1.0952 | 1.7687 | 1.7676 | | 2.5234 | 3.0756 | 3.1233 | 2.6216 | H7 | 2.0753 | 1.0946 | 2.1599 | 2.5123 | 3.0756 | 2.5234 | | 1.7490 | 2.9250 | 2.3882 | H8 | 2.0753 | 1.0946 | 2.1599 | 2.5123 | 2.5234 | 3.0756 | 1.7490 | | 2.3882 | 2.9250 | H9 | 1.0159 | 2.0444 | 2.7473 | 3.7451 | 2.6216 | 3.1233 | 2.9250 | 2.3882 | | 1.6308 | H10 | 1.0159 | 2.0444 | 2.7473 | 3.7451 | 3.1233 | 2.6216 | 2.3882 | 2.9250 | 1.6308 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.958 |
|
N1 |
C2 |
H7 |
107.322 |
| N1 |
C2 |
H8 |
107.322 |
|
C2 |
N1 |
H9 |
109.503 |
| C2 |
N1 |
H10 |
109.503 |
|
C2 |
C3 |
H4 |
111.854 |
| C2 |
C3 |
H5 |
110.984 |
|
C2 |
C3 |
H6 |
110.984 |
| C3 |
C2 |
H7 |
109.848 |
|
C3 |
C2 |
H8 |
109.848 |
| H4 |
C3 |
H5 |
107.614 |
|
H4 |
C3 |
H6 |
107.614 |
| H5 |
C3 |
H6 |
107.600 |
|
H7 |
C2 |
H8 |
106.054 |
| H9 |
N1 |
H10 |
106.759 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.727 |
|
|
|
| 2 |
C |
-0.144 |
|
|
|
| 3 |
C |
-0.462 |
|
|
|
| 4 |
H |
0.148 |
|
|
|
| 5 |
H |
0.143 |
|
|
|
| 6 |
H |
0.143 |
|
|
|
| 7 |
H |
0.151 |
|
|
|
| 8 |
H |
0.151 |
|
|
|
| 9 |
H |
0.299 |
|
|
|
| 10 |
H |
0.299 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.020 |
-1.067 |
0.000 |
1.476 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.112 |
2.668 |
0.000 |
| y |
2.668 |
-20.138 |
0.000 |
| z |
0.000 |
0.000 |
-19.094 |
|
| Traceless |
| | x | y | z |
| x |
-4.496 |
2.668 |
0.000 |
| y |
2.668 |
1.465 |
0.000 |
| z |
0.000 |
0.000 |
3.031 |
|
| Polar |
| 3z2-r2 | 6.062 |
| x2-y2 | -3.974 |
| xy | 2.668 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.582 |
0.269 |
0.000 |
| y |
0.269 |
4.189 |
0.000 |
| z |
0.000 |
0.000 |
4.275 |
<r2> (average value of r
2) Å
2
| <r2> |
58.646 |
| (<r2>)1/2 |
7.658 |
Jump to
S1C1
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -134.992480 |
| 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 B2PLYP/6-31G*
Geometric Data calculated at B2PLYP/6-31G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability