Jump to
S1C2
Energy calculated at HF/Def2TZVPP
| hartrees |
Energy at 0K | -134.309447 |
Energy at 298.15K | -134.317756 |
HF Energy | -134.309447 |
Nuclear repulsion energy | 83.338844 |
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 HF/Def2TZVPP
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' |
3720 |
3372 |
0.48 |
|
|
|
2 |
A' |
3207 |
2907 |
73.45 |
|
|
|
3 |
A' |
3168 |
2872 |
31.81 |
|
|
|
4 |
A' |
3145 |
2851 |
32.93 |
|
|
|
5 |
A' |
1794 |
1626 |
26.74 |
|
|
|
6 |
A' |
1627 |
1475 |
1.42 |
|
|
|
7 |
A' |
1605 |
1455 |
0.55 |
|
|
|
8 |
A' |
1535 |
1391 |
11.31 |
|
|
|
9 |
A' |
1501 |
1360 |
13.11 |
|
|
|
10 |
A' |
1232 |
1116 |
12.53 |
|
|
|
11 |
A' |
1143 |
1036 |
39.83 |
|
|
|
12 |
A' |
953 |
864 |
38.30 |
|
|
|
13 |
A' |
916 |
831 |
138.56 |
|
|
|
14 |
A' |
431 |
390 |
6.62 |
|
|
|
15 |
A" |
3797 |
3442 |
1.18 |
|
|
|
16 |
A" |
3215 |
2914 |
98.49 |
|
|
|
17 |
A" |
3184 |
2886 |
0.04 |
|
|
|
18 |
A" |
1608 |
1457 |
6.08 |
|
|
|
19 |
A" |
1498 |
1358 |
0.20 |
|
|
|
20 |
A" |
1374 |
1246 |
0.03 |
|
|
|
21 |
A" |
1078 |
977 |
0.78 |
|
|
|
22 |
A" |
834 |
756 |
0.43 |
|
|
|
23 |
A" |
302 |
274 |
25.80 |
|
|
|
24 |
A" |
264 |
239 |
22.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21565.1 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 19546.6 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 HF/Def2TZVPP
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-1.297 |
-0.091 |
0.000 |
C2 |
0.000 |
0.571 |
0.000 |
C3 |
1.207 |
-0.351 |
0.000 |
H4 |
2.135 |
0.211 |
0.000 |
H5 |
1.209 |
-0.991 |
0.876 |
H6 |
1.209 |
-0.991 |
-0.876 |
H7 |
0.036 |
1.221 |
-0.866 |
H8 |
0.036 |
1.221 |
0.866 |
H9 |
-1.395 |
-0.675 |
0.804 |
H10 |
-1.395 |
-0.675 |
-0.804 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
N1 | | 1.4565 | 2.5176 | 3.4457 | 2.8032 | 2.8032 | 2.0611 | 2.0611 | 0.9980 | 0.9980 |
C2 | 1.4565 | | 1.5194 | 2.1656 | 2.1613 | 2.1613 | 1.0827 | 1.0827 | 2.0360 | 2.0360 | C3 | 2.5176 | 1.5194 | | 1.0854 | 1.0849 | 1.0849 | 2.1429 | 2.1429 | 2.7429 | 2.7429 | H4 | 3.4457 | 2.1656 | 1.0854 | | 1.7526 | 1.7526 | 2.4850 | 2.4850 | 3.7278 | 3.7278 | H5 | 2.8032 | 2.1613 | 1.0849 | 1.7526 | | 1.7518 | 3.0499 | 2.5039 | 2.6246 | 3.1152 | H6 | 2.8032 | 2.1613 | 1.0849 | 1.7526 | 1.7518 | | 2.5039 | 3.0499 | 3.1152 | 2.6246 | H7 | 2.0611 | 1.0827 | 2.1429 | 2.4850 | 3.0499 | 2.5039 | | 1.7311 | 2.9032 | 2.3761 | H8 | 2.0611 | 1.0827 | 2.1429 | 2.4850 | 2.5039 | 3.0499 | 1.7311 | | 2.3761 | 2.9032 | H9 | 0.9980 | 2.0360 | 2.7429 | 3.7278 | 2.6246 | 3.1152 | 2.9032 | 2.3761 | | 1.6074 | H10 | 0.9980 | 2.0360 | 2.7429 | 3.7278 | 3.1152 | 2.6246 | 2.3761 | 2.9032 | 1.6074 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
C2 |
C3 |
115.548 |
|
N1 |
C2 |
H7 |
107.615 |
N1 |
C2 |
H8 |
107.615 |
|
C2 |
N1 |
H9 |
110.712 |
C2 |
N1 |
H10 |
110.712 |
|
C2 |
C3 |
H4 |
111.394 |
C2 |
C3 |
H5 |
111.082 |
|
C2 |
C3 |
H6 |
111.082 |
C3 |
C2 |
H7 |
109.738 |
|
C3 |
C2 |
H8 |
109.738 |
H4 |
C3 |
H5 |
107.712 |
|
H4 |
C3 |
H6 |
107.712 |
H5 |
C3 |
H6 |
107.685 |
|
H7 |
C2 |
H8 |
106.151 |
H9 |
N1 |
H10 |
107.277 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/Def2TZVPP
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.392 |
|
|
|
2 |
C |
0.111 |
|
|
|
3 |
C |
-0.163 |
|
|
|
4 |
H |
0.046 |
|
|
|
5 |
H |
0.038 |
|
|
|
6 |
H |
0.038 |
|
|
|
7 |
H |
0.034 |
|
|
|
8 |
H |
0.034 |
|
|
|
9 |
H |
0.126 |
|
|
|
10 |
H |
0.126 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.930 |
-0.928 |
0.000 |
1.314 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.042 |
2.650 |
0.000 |
y |
2.650 |
-20.480 |
0.000 |
z |
0.000 |
0.000 |
-19.102 |
|
Traceless |
| x | y | z |
x |
-4.251 |
2.650 |
0.000 |
y |
2.650 |
1.092 |
0.000 |
z |
0.000 |
0.000 |
3.159 |
|
Polar |
3z2-r2 | 6.318 |
x2-y2 | -3.562 |
xy | 2.650 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.279 |
0.081 |
0.000 |
y |
0.081 |
4.803 |
0.000 |
z |
0.000 |
0.000 |
4.668 |
<r2> (average value of r
2) Å
2
<r2> |
58.193 |
(<r2>)1/2 |
7.628 |
Jump to
S1C1
Energy calculated at HF/Def2TZVPP
| hartrees |
Energy at 0K | -134.309675 |
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 HF/Def2TZVPP
Geometric Data calculated at HF/Def2TZVPP
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability