Jump to
S1C2
Energy calculated at mPW1PW91/6-31+G**
| | hartrees |
| Energy at 0K | -135.154106 |
| Energy at 298.15K | -135.162252 |
| Nuclear repulsion energy | 82.829554 |
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 mPW1PW91/6-31+G**
| 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' |
3550 |
3379 |
0.51 |
|
|
|
| 2 |
A' |
3134 |
2983 |
42.67 |
|
|
|
| 3 |
A' |
3070 |
2922 |
36.38 |
|
|
|
| 4 |
A' |
3051 |
2904 |
26.70 |
|
|
|
| 5 |
A' |
1679 |
1598 |
33.54 |
|
|
|
| 6 |
A' |
1511 |
1438 |
4.34 |
|
|
|
| 7 |
A' |
1494 |
1422 |
0.21 |
|
|
|
| 8 |
A' |
1418 |
1350 |
16.16 |
|
|
|
| 9 |
A' |
1385 |
1318 |
11.56 |
|
|
|
| 10 |
A' |
1160 |
1105 |
12.98 |
|
|
|
| 11 |
A' |
1088 |
1036 |
30.03 |
|
|
|
| 12 |
A' |
900 |
857 |
5.69 |
|
|
|
| 13 |
A' |
839 |
799 |
197.12 |
|
|
|
| 14 |
A' |
405 |
386 |
8.72 |
|
|
|
| 15 |
A" |
3644 |
3469 |
1.75 |
|
|
|
| 16 |
A" |
3139 |
2988 |
57.76 |
|
|
|
| 17 |
A" |
3107 |
2957 |
5.22 |
|
|
|
| 18 |
A" |
1502 |
1429 |
10.01 |
|
|
|
| 19 |
A" |
1395 |
1328 |
0.12 |
|
|
|
| 20 |
A" |
1273 |
1212 |
0.00 |
|
|
|
| 21 |
A" |
1008 |
960 |
1.16 |
|
|
|
| 22 |
A" |
780 |
742 |
1.19 |
|
|
|
| 23 |
A" |
293 |
279 |
39.16 |
|
|
|
| 24 |
A" |
252 |
240 |
18.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20538.7 cm
-1
Scaled (by 0.9518) Zero Point Vibrational Energy (zpe) 19548.7 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 mPW1PW91/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.303 |
-0.083 |
0.000 |
| C2 |
0.000 |
0.569 |
0.000 |
| C3 |
1.214 |
-0.357 |
0.000 |
| H4 |
2.150 |
0.212 |
0.000 |
| H5 |
1.215 |
-1.003 |
0.884 |
| H6 |
1.215 |
-1.003 |
-0.884 |
| H7 |
0.040 |
1.228 |
-0.874 |
| H8 |
0.040 |
1.228 |
0.874 |
| H9 |
-1.412 |
-0.675 |
0.816 |
| H10 |
-1.412 |
-0.675 |
-0.816 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4568 | 2.5314 | 3.4647 | 2.8226 | 2.8226 | 2.0698 | 2.0698 | 1.0138 | 1.0138 |
C2 | 1.4568 | | 1.5272 | 2.1791 | 2.1751 | 2.1751 | 1.0952 | 1.0952 | 2.0512 | 2.0512 | C3 | 2.5314 | 1.5272 | | 1.0950 | 1.0950 | 1.0950 | 2.1578 | 2.1578 | 2.7681 | 2.7681 | H4 | 3.4647 | 2.1791 | 1.0950 | | 1.7695 | 1.7695 | 2.4998 | 2.4998 | 3.7599 | 3.7599 | H5 | 2.8226 | 2.1751 | 1.0950 | 1.7695 | | 1.7684 | 3.0744 | 2.5219 | 2.6485 | 3.1464 | H6 | 2.8226 | 2.1751 | 1.0950 | 1.7695 | 1.7684 | | 2.5219 | 3.0744 | 3.1464 | 2.6485 | H7 | 2.0698 | 1.0952 | 2.1578 | 2.4998 | 3.0744 | 2.5219 | | 1.7486 | 2.9298 | 2.3938 | H8 | 2.0698 | 1.0952 | 2.1578 | 2.4998 | 2.5219 | 3.0744 | 1.7486 | | 2.3938 | 2.9298 | H9 | 1.0138 | 2.0512 | 2.7681 | 3.7599 | 2.6485 | 3.1464 | 2.9298 | 2.3938 | | 1.6316 | H10 | 1.0138 | 2.0512 | 2.7681 | 3.7599 | 3.1464 | 2.6485 | 2.3938 | 2.9298 | 1.6316 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.039 |
|
N1 |
C2 |
H7 |
107.547 |
| N1 |
C2 |
H8 |
107.547 |
|
C2 |
N1 |
H9 |
110.978 |
| C2 |
N1 |
H10 |
110.978 |
|
C2 |
C3 |
H4 |
111.338 |
| C2 |
C3 |
H5 |
111.024 |
|
C2 |
C3 |
H6 |
111.024 |
| C3 |
C2 |
H7 |
109.641 |
|
C3 |
C2 |
H8 |
109.641 |
| H4 |
C3 |
H5 |
107.797 |
|
H4 |
C3 |
H6 |
107.797 |
| H5 |
C3 |
H6 |
107.698 |
|
H7 |
C2 |
H8 |
105.932 |
| H9 |
N1 |
H10 |
107.170 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.617 |
|
|
|
| 2 |
C |
-0.252 |
|
|
|
| 3 |
C |
-0.537 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
| 5 |
H |
0.163 |
|
|
|
| 6 |
H |
0.163 |
|
|
|
| 7 |
H |
0.163 |
|
|
|
| 8 |
H |
0.163 |
|
|
|
| 9 |
H |
0.294 |
|
|
|
| 10 |
H |
0.294 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.045 |
-0.999 |
0.000 |
1.446 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
58.799 |
| (<r2>)1/2 |
7.668 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31+G**
| | hartrees |
| Energy at 0K | -135.155194 |
| 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 mPW1PW91/6-31+G**
Geometric Data calculated at mPW1PW91/6-31+G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability