Jump to
S1C2
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -134.396195 |
| Energy at 298.15K | -134.404329 |
| Nuclear repulsion energy | 82.284862 |
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 mPW1PW91/3-21G*
| 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' |
3451 |
3277 |
1.42 |
|
|
|
| 2 |
A' |
3138 |
2979 |
37.87 |
|
|
|
| 3 |
A' |
3080 |
2925 |
29.40 |
|
|
|
| 4 |
A' |
3060 |
2906 |
19.08 |
|
|
|
| 5 |
A' |
1732 |
1645 |
20.62 |
|
|
|
| 6 |
A' |
1566 |
1487 |
4.63 |
|
|
|
| 7 |
A' |
1547 |
1469 |
1.74 |
|
|
|
| 8 |
A' |
1455 |
1382 |
8.27 |
|
|
|
| 9 |
A' |
1406 |
1335 |
5.70 |
|
|
|
| 10 |
A' |
1170 |
1111 |
13.74 |
|
|
|
| 11 |
A' |
1054 |
1001 |
8.48 |
|
|
|
| 12 |
A' |
900 |
855 |
17.60 |
|
|
|
| 13 |
A' |
714 |
678 |
265.39 |
|
|
|
| 14 |
A' |
395 |
375 |
8.67 |
|
|
|
| 15 |
A" |
3552 |
3373 |
0.24 |
|
|
|
| 16 |
A" |
3145 |
2987 |
51.90 |
|
|
|
| 17 |
A" |
3114 |
2957 |
1.21 |
|
|
|
| 18 |
A" |
1566 |
1488 |
10.21 |
|
|
|
| 19 |
A" |
1417 |
1346 |
0.10 |
|
|
|
| 20 |
A" |
1306 |
1240 |
0.04 |
|
|
|
| 21 |
A" |
1031 |
979 |
1.71 |
|
|
|
| 22 |
A" |
794 |
754 |
3.22 |
|
|
|
| 23 |
A" |
312 |
296 |
54.90 |
|
|
|
| 24 |
A" |
258 |
245 |
10.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20580.7 cm
-1
Scaled (by 0.9496) Zero Point Vibrational Energy (zpe) 19543.4 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 mPW1PW91/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.305 |
-0.103 |
0.000 |
| C2 |
0.000 |
0.582 |
0.000 |
| C3 |
1.224 |
-0.352 |
0.000 |
| H4 |
2.160 |
0.217 |
0.000 |
| H5 |
1.213 |
-0.994 |
0.888 |
| H6 |
1.213 |
-0.994 |
-0.888 |
| H7 |
0.035 |
1.234 |
-0.880 |
| H8 |
0.035 |
1.234 |
0.880 |
| H9 |
-1.431 |
-0.679 |
0.834 |
| H10 |
-1.431 |
-0.679 |
-0.834 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4744 | 2.5418 | 3.4806 | 2.8148 | 2.8148 | 2.0872 | 2.0872 | 1.0216 | 1.0216 |
C2 | 1.4744 | | 1.5400 | 2.1911 | 2.1783 | 2.1783 | 1.0951 | 1.0951 | 2.0819 | 2.0819 | C3 | 2.5418 | 1.5400 | | 1.0957 | 1.0960 | 1.0960 | 2.1687 | 2.1687 | 2.8022 | 2.8022 | H4 | 3.4806 | 2.1911 | 1.0957 | | 1.7762 | 1.7762 | 2.5152 | 2.5152 | 3.7943 | 3.7943 | H5 | 2.8148 | 2.1783 | 1.0960 | 1.7762 | | 1.7757 | 3.0784 | 2.5203 | 2.6627 | 3.1707 | H6 | 2.8148 | 2.1783 | 1.0960 | 1.7762 | 1.7757 | | 2.5203 | 3.0784 | 3.1707 | 2.6627 | H7 | 2.0872 | 1.0951 | 2.1687 | 2.5152 | 3.0784 | 2.5203 | | 1.7596 | 2.9570 | 2.4098 | H8 | 2.0872 | 1.0951 | 2.1687 | 2.5152 | 2.5203 | 3.0784 | 1.7596 | | 2.4098 | 2.9570 | H9 | 1.0216 | 2.0819 | 2.8022 | 3.7943 | 2.6627 | 3.1707 | 2.9570 | 2.4098 | | 1.6690 | H10 | 1.0216 | 2.0819 | 2.8022 | 3.7943 | 3.1707 | 2.6627 | 2.4098 | 2.9570 | 1.6690 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
114.944 |
|
N1 |
C2 |
H7 |
107.722 |
| N1 |
C2 |
H8 |
107.722 |
|
C2 |
N1 |
H9 |
111.762 |
| C2 |
N1 |
H10 |
111.762 |
|
C2 |
C3 |
H4 |
111.351 |
| C2 |
C3 |
H5 |
110.319 |
|
C2 |
C3 |
H6 |
110.319 |
| C3 |
C2 |
H7 |
109.615 |
|
C3 |
C2 |
H8 |
109.615 |
| H4 |
C3 |
H5 |
108.274 |
|
H4 |
C3 |
H6 |
108.274 |
| H5 |
C3 |
H6 |
108.210 |
|
H7 |
C2 |
H8 |
106.904 |
| H9 |
N1 |
H10 |
109.540 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.691 |
|
|
|
| 2 |
C |
-0.292 |
|
|
|
| 3 |
C |
-0.643 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
0.205 |
|
|
|
| 6 |
H |
0.205 |
|
|
|
| 7 |
H |
0.226 |
|
|
|
| 8 |
H |
0.226 |
|
|
|
| 9 |
H |
0.278 |
|
|
|
| 10 |
H |
0.278 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.910 |
-1.102 |
0.000 |
1.429 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.551 |
2.849 |
0.000 |
| y |
2.849 |
-19.814 |
0.000 |
| z |
0.000 |
0.000 |
-18.735 |
|
| Traceless |
| | x | y | z |
| x |
-4.276 |
2.849 |
0.000 |
| y |
2.849 |
1.328 |
0.000 |
| z |
0.000 |
0.000 |
2.948 |
|
| Polar |
| 3z2-r2 | 5.896 |
| x2-y2 | -3.736 |
| xy | 2.849 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.283 |
0.341 |
0.000 |
| y |
0.341 |
3.813 |
0.000 |
| z |
0.000 |
0.000 |
4.025 |
<r2> (average value of r
2) Å
2
| <r2> |
58.917 |
| (<r2>)1/2 |
7.676 |
Jump to
S1C1
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -134.395059 |
| 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 mPW1PW91/3-21G*
Geometric Data calculated at mPW1PW91/3-21G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability