Jump to
S1C2
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -135.095188 |
| Energy at 298.15K | -135.103368 |
| Nuclear repulsion energy | 82.811614 |
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 B1B95/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' |
3481 |
3346 |
1.72 |
|
|
|
| 2 |
A' |
3125 |
3004 |
39.47 |
|
|
|
| 3 |
A' |
3050 |
2932 |
36.29 |
|
|
|
| 4 |
A' |
3039 |
2921 |
27.88 |
|
|
|
| 5 |
A' |
1649 |
1585 |
15.56 |
|
|
|
| 6 |
A' |
1475 |
1417 |
1.68 |
|
|
|
| 7 |
A' |
1455 |
1399 |
0.04 |
|
|
|
| 8 |
A' |
1388 |
1334 |
14.70 |
|
|
|
| 9 |
A' |
1360 |
1307 |
13.31 |
|
|
|
| 10 |
A' |
1162 |
1117 |
7.53 |
|
|
|
| 11 |
A' |
1088 |
1046 |
31.85 |
|
|
|
| 12 |
A' |
903 |
868 |
53.19 |
|
|
|
| 13 |
A' |
886 |
852 |
99.47 |
|
|
|
| 14 |
A' |
394 |
379 |
5.69 |
|
|
|
| 15 |
A" |
3558 |
3420 |
0.15 |
|
|
|
| 16 |
A" |
3128 |
3007 |
50.34 |
|
|
|
| 17 |
A" |
3088 |
2968 |
11.28 |
|
|
|
| 18 |
A" |
1460 |
1404 |
7.95 |
|
|
|
| 19 |
A" |
1384 |
1331 |
0.00 |
|
|
|
| 20 |
A" |
1258 |
1209 |
0.09 |
|
|
|
| 21 |
A" |
1002 |
963 |
1.26 |
|
|
|
| 22 |
A" |
774 |
744 |
1.56 |
|
|
|
| 23 |
A" |
310 |
298 |
36.35 |
|
|
|
| 24 |
A" |
259 |
249 |
8.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20338.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 19549.1 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 B1B95/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.306 |
-0.074 |
0.000 |
| C2 |
0.000 |
0.571 |
0.000 |
| C3 |
1.205 |
-0.361 |
0.000 |
| H4 |
2.153 |
0.199 |
0.000 |
| H5 |
1.201 |
-1.011 |
0.889 |
| H6 |
1.201 |
-1.011 |
-0.889 |
| H7 |
0.047 |
1.235 |
-0.878 |
| H8 |
0.047 |
1.235 |
0.878 |
| H9 |
-1.369 |
-0.695 |
0.808 |
| H10 |
-1.369 |
-0.695 |
-0.808 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4566 | 2.5274 | 3.4697 | 2.8200 | 2.8200 | 2.0772 | 2.0772 | 1.0209 | 1.0209 |
C2 | 1.4566 | | 1.5233 | 2.1848 | 2.1760 | 2.1760 | 1.1017 | 1.1017 | 2.0321 | 2.0321 | C3 | 2.5274 | 1.5233 | | 1.1007 | 1.1012 | 1.1012 | 2.1584 | 2.1584 | 2.7183 | 2.7183 | H4 | 3.4697 | 2.1848 | 1.1007 | | 1.7777 | 1.7777 | 2.5059 | 2.5059 | 3.7222 | 3.7222 | H5 | 2.8200 | 2.1760 | 1.1012 | 1.7777 | | 1.7771 | 3.0818 | 2.5253 | 2.5904 | 3.0953 | H6 | 2.8200 | 2.1760 | 1.1012 | 1.7777 | 1.7771 | | 2.5253 | 3.0818 | 3.0953 | 2.5904 | H7 | 2.0772 | 1.1017 | 2.1584 | 2.5059 | 3.0818 | 2.5253 | | 1.7558 | 2.9277 | 2.3948 | H8 | 2.0772 | 1.1017 | 2.1584 | 2.5059 | 2.5253 | 3.0818 | 1.7558 | | 2.3948 | 2.9277 | H9 | 1.0209 | 2.0321 | 2.7183 | 3.7222 | 2.5904 | 3.0953 | 2.9277 | 2.3948 | | 1.6153 | H10 | 1.0209 | 2.0321 | 2.7183 | 3.7222 | 3.0953 | 2.5904 | 2.3948 | 2.9277 | 1.6153 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.004 |
|
N1 |
C2 |
H7 |
107.761 |
| N1 |
C2 |
H8 |
107.761 |
|
C2 |
N1 |
H9 |
108.947 |
| C2 |
N1 |
H10 |
108.947 |
|
C2 |
C3 |
H4 |
111.729 |
| C2 |
C3 |
H5 |
110.998 |
|
C2 |
C3 |
H6 |
110.998 |
| C3 |
C2 |
H7 |
109.572 |
|
C3 |
C2 |
H8 |
109.572 |
| H4 |
C3 |
H5 |
107.672 |
|
H4 |
C3 |
H6 |
107.672 |
| H5 |
C3 |
H6 |
107.588 |
|
H7 |
C2 |
H8 |
105.657 |
| H9 |
N1 |
H10 |
104.583 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.202 |
|
|
|
| 2 |
C |
-0.015 |
|
|
|
| 3 |
C |
-0.069 |
|
|
|
| 4 |
H |
0.025 |
|
|
|
| 5 |
H |
0.024 |
|
|
|
| 6 |
H |
0.024 |
|
|
|
| 7 |
H |
0.031 |
|
|
|
| 8 |
H |
0.031 |
|
|
|
| 9 |
H |
0.076 |
|
|
|
| 10 |
H |
0.076 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.801 |
-0.946 |
0.000 |
1.240 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.459 |
2.430 |
0.000 |
| y |
2.430 |
-20.064 |
0.000 |
| z |
0.000 |
0.000 |
-19.087 |
|
| Traceless |
| | x | y | z |
| x |
-3.884 |
2.430 |
0.000 |
| y |
2.430 |
1.209 |
0.000 |
| z |
0.000 |
0.000 |
2.675 |
|
| Polar |
| 3z2-r2 | 5.350 |
| x2-y2 | -3.395 |
| xy | 2.430 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.013 |
0.185 |
0.000 |
| y |
0.185 |
4.575 |
0.000 |
| z |
0.000 |
0.000 |
4.493 |
<r2> (average value of r
2) Å
2
| <r2> |
58.261 |
| (<r2>)1/2 |
7.633 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVDZ
| | hartrees |
| Energy at 0K | -135.094313 |
| 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 B1B95/cc-pVDZ
Geometric Data calculated at B1B95/cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability