Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -135.129024 |
| Energy at 298.15K | -135.137180 |
| Nuclear repulsion energy | 82.991233 |
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 B1B95/6-311G**
| 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' |
3508 |
3368 |
1.27 |
|
|
|
| 2 |
A' |
3110 |
2986 |
48.34 |
|
|
|
| 3 |
A' |
3048 |
2926 |
37.98 |
|
|
|
| 4 |
A' |
3032 |
2911 |
24.90 |
|
|
|
| 5 |
A' |
1663 |
1597 |
23.57 |
|
|
|
| 6 |
A' |
1500 |
1440 |
3.11 |
|
|
|
| 7 |
A' |
1481 |
1422 |
0.16 |
|
|
|
| 8 |
A' |
1402 |
1346 |
12.88 |
|
|
|
| 9 |
A' |
1374 |
1319 |
11.09 |
|
|
|
| 10 |
A' |
1157 |
1111 |
8.66 |
|
|
|
| 11 |
A' |
1079 |
1036 |
29.74 |
|
|
|
| 12 |
A' |
896 |
860 |
26.49 |
|
|
|
| 13 |
A' |
864 |
830 |
157.75 |
|
|
|
| 14 |
A' |
394 |
378 |
6.84 |
|
|
|
| 15 |
A" |
3587 |
3444 |
0.06 |
|
|
|
| 16 |
A" |
3113 |
2989 |
64.59 |
|
|
|
| 17 |
A" |
3078 |
2956 |
6.28 |
|
|
|
| 18 |
A" |
1488 |
1429 |
9.06 |
|
|
|
| 19 |
A" |
1392 |
1336 |
0.00 |
|
|
|
| 20 |
A" |
1266 |
1216 |
0.08 |
|
|
|
| 21 |
A" |
1006 |
965 |
1.13 |
|
|
|
| 22 |
A" |
775 |
744 |
1.11 |
|
|
|
| 23 |
A" |
300 |
288 |
37.08 |
|
|
|
| 24 |
A" |
251 |
241 |
11.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20382.3 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 19569.0 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.303 |
-0.081 |
0.000 |
| C2 |
0.000 |
0.572 |
0.000 |
| C3 |
1.208 |
-0.358 |
0.000 |
| H4 |
2.148 |
0.200 |
0.000 |
| H5 |
1.202 |
-1.003 |
0.882 |
| H6 |
1.202 |
-1.003 |
-0.882 |
| H7 |
0.042 |
1.230 |
-0.872 |
| H8 |
0.042 |
1.230 |
0.872 |
| H9 |
-1.382 |
-0.686 |
0.810 |
| H10 |
-1.382 |
-0.686 |
-0.810 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4573 | 2.5253 | 3.4616 | 2.8109 | 2.8109 | 2.0705 | 2.0705 | 1.0139 | 1.0139 |
C2 | 1.4573 | | 1.5242 | 2.1796 | 2.1691 | 2.1691 | 1.0934 | 1.0934 | 2.0368 | 2.0368 | C3 | 2.5253 | 1.5242 | | 1.0930 | 1.0932 | 1.0932 | 2.1545 | 2.1545 | 2.7328 | 2.7328 | H4 | 3.4616 | 2.1796 | 1.0930 | | 1.7663 | 1.7663 | 2.5015 | 2.5015 | 3.7279 | 3.7279 | H5 | 2.8109 | 2.1691 | 1.0932 | 1.7663 | | 1.7648 | 3.0680 | 2.5167 | 2.6042 | 3.1048 | H6 | 2.8109 | 2.1691 | 1.0932 | 1.7663 | 1.7648 | | 2.5167 | 3.0680 | 3.1048 | 2.6042 | H7 | 2.0705 | 1.0934 | 2.1545 | 2.5015 | 3.0680 | 2.5167 | | 1.7446 | 2.9202 | 2.3878 | H8 | 2.0705 | 1.0934 | 2.1545 | 2.5015 | 2.5167 | 3.0680 | 1.7446 | | 2.3878 | 2.9202 | H9 | 1.0139 | 2.0368 | 2.7328 | 3.7279 | 2.6042 | 3.1048 | 2.9202 | 2.3878 | | 1.6196 | H10 | 1.0139 | 2.0368 | 2.7328 | 3.7279 | 3.1048 | 2.6042 | 2.3878 | 2.9202 | 1.6196 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
115.759 |
|
N1 |
C2 |
H7 |
107.685 |
| N1 |
C2 |
H8 |
107.685 |
|
C2 |
N1 |
H9 |
109.716 |
| C2 |
N1 |
H10 |
109.716 |
|
C2 |
C3 |
H4 |
111.719 |
| C2 |
C3 |
H5 |
110.862 |
|
C2 |
C3 |
H6 |
110.862 |
| C3 |
C2 |
H7 |
109.695 |
|
C3 |
C2 |
H8 |
109.695 |
| H4 |
C3 |
H5 |
107.793 |
|
H4 |
C3 |
H6 |
107.793 |
| H5 |
C3 |
H6 |
107.642 |
|
H7 |
C2 |
H8 |
105.844 |
| H9 |
N1 |
H10 |
106.016 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.460 |
|
|
|
| 2 |
C |
-0.171 |
|
|
|
| 3 |
C |
-0.346 |
|
|
|
| 4 |
H |
0.116 |
|
|
|
| 5 |
H |
0.110 |
|
|
|
| 6 |
H |
0.110 |
|
|
|
| 7 |
H |
0.130 |
|
|
|
| 8 |
H |
0.130 |
|
|
|
| 9 |
H |
0.191 |
|
|
|
| 10 |
H |
0.191 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.882 |
-0.947 |
0.000 |
1.294 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.839 |
2.607 |
0.000 |
| y |
2.607 |
-20.284 |
0.000 |
| z |
0.000 |
0.000 |
-19.117 |
|
| Traceless |
| | x | y | z |
| x |
-4.139 |
2.607 |
0.000 |
| y |
2.607 |
1.194 |
0.000 |
| z |
0.000 |
0.000 |
2.944 |
|
| Polar |
| 3z2-r2 | 5.889 |
| x2-y2 | -3.555 |
| xy | 2.607 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.236 |
0.135 |
0.000 |
| y |
0.135 |
4.730 |
0.000 |
| z |
0.000 |
0.000 |
4.640 |
<r2> (average value of r
2) Å
2
| <r2> |
58.305 |
| (<r2>)1/2 |
7.636 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -135.127833 |
| 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 B1B95/6-311G**
Geometric Data calculated at B1B95/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability