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S1C2
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -133.504146 |
Energy at 298.15K | -133.512393 |
Nuclear repulsion energy | 82.625112 |
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/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' |
3663 |
3307 |
0.35 |
|
|
|
2 |
A' |
3252 |
2936 |
53.44 |
|
|
|
3 |
A' |
3220 |
2906 |
26.33 |
|
|
|
4 |
A' |
3188 |
2877 |
23.69 |
|
|
|
5 |
A' |
1847 |
1667 |
24.30 |
|
|
|
6 |
A' |
1673 |
1510 |
3.54 |
|
|
|
7 |
A' |
1660 |
1498 |
0.26 |
|
|
|
8 |
A' |
1565 |
1413 |
5.66 |
|
|
|
9 |
A' |
1511 |
1363 |
7.75 |
|
|
|
10 |
A' |
1235 |
1115 |
16.93 |
|
|
|
11 |
A' |
1089 |
983 |
15.11 |
|
|
|
12 |
A' |
933 |
842 |
24.86 |
|
|
|
13 |
A' |
767 |
692 |
288.51 |
|
|
|
14 |
A' |
423 |
382 |
8.46 |
|
|
|
15 |
A" |
3760 |
3394 |
0.25 |
|
|
|
16 |
A" |
3267 |
2949 |
68.99 |
|
|
|
17 |
A" |
3235 |
2920 |
3.18 |
|
|
|
18 |
A" |
1668 |
1506 |
7.24 |
|
|
|
19 |
A" |
1507 |
1361 |
0.01 |
|
|
|
20 |
A" |
1390 |
1255 |
0.18 |
|
|
|
21 |
A" |
1087 |
982 |
0.78 |
|
|
|
22 |
A" |
846 |
764 |
1.74 |
|
|
|
23 |
A" |
309 |
279 |
50.28 |
|
|
|
24 |
A" |
258 |
233 |
15.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21677.0 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 19565.7 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 HF/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
-1.298 |
-0.111 |
0.000 |
C2 |
0.000 |
0.585 |
0.000 |
C3 |
1.226 |
-0.352 |
0.000 |
H4 |
2.150 |
0.215 |
0.000 |
H5 |
1.215 |
-0.988 |
0.879 |
H6 |
1.215 |
-0.988 |
-0.879 |
H7 |
0.032 |
1.227 |
-0.871 |
H8 |
0.032 |
1.227 |
0.871 |
H9 |
-1.457 |
-0.657 |
0.828 |
H10 |
-1.457 |
-0.657 |
-0.828 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
N1 | | 1.4726 | 2.5355 | 3.4638 | 2.8037 | 2.8037 | 2.0773 | 2.0773 | 1.0047 | 1.0047 |
C2 | 1.4726 | | 1.5431 | 2.1820 | 2.1737 | 2.1737 | 1.0826 | 1.0826 | 2.0859 | 2.0859 | C3 | 2.5355 | 1.5431 | | 1.0847 | 1.0852 | 1.0852 | 2.1630 | 2.1630 | 2.8246 | 2.8246 | H4 | 3.4638 | 2.1820 | 1.0847 | | 1.7593 | 1.7593 | 2.5044 | 2.5044 | 3.8028 | 3.8028 | H5 | 2.8037 | 2.1737 | 1.0852 | 1.7593 | | 1.7585 | 3.0613 | 2.5114 | 2.6937 | 3.1888 | H6 | 2.8037 | 2.1737 | 1.0852 | 1.7593 | 1.7585 | | 2.5114 | 3.0613 | 3.1888 | 2.6937 | H7 | 2.0773 | 1.0826 | 2.1630 | 2.5044 | 3.0613 | 2.5114 | | 1.7426 | 2.9414 | 2.4012 | H8 | 2.0773 | 1.0826 | 2.1630 | 2.5044 | 2.5114 | 3.0613 | 1.7426 | | 2.4012 | 2.9414 | H9 | 1.0047 | 2.0859 | 2.8246 | 3.8028 | 2.6937 | 3.1888 | 2.9414 | 2.4012 | | 1.6562 | H10 | 1.0047 | 2.0859 | 2.8246 | 3.8028 | 3.1888 | 2.6937 | 2.4012 | 2.9414 | 1.6562 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
C2 |
C3 |
114.421 |
|
N1 |
C2 |
H7 |
107.802 |
N1 |
C2 |
H8 |
107.802 |
|
C2 |
N1 |
H9 |
113.360 |
C2 |
N1 |
H10 |
113.360 |
|
C2 |
C3 |
H4 |
111.071 |
C2 |
C3 |
H5 |
110.378 |
|
C2 |
C3 |
H6 |
110.378 |
C3 |
C2 |
H7 |
109.683 |
|
C3 |
C2 |
H8 |
109.683 |
H4 |
C3 |
H5 |
108.345 |
|
H4 |
C3 |
H6 |
108.345 |
H5 |
C3 |
H6 |
108.238 |
|
H7 |
C2 |
H8 |
107.184 |
H9 |
N1 |
H10 |
111.024 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.781 |
-0.361 |
|
|
2 |
C |
-0.209 |
0.056 |
|
|
3 |
C |
-0.608 |
0.103 |
|
|
4 |
H |
0.196 |
0.098 |
|
|
5 |
H |
0.194 |
-1.136 |
|
|
6 |
H |
0.194 |
-0.029 |
|
|
7 |
H |
0.215 |
-0.085 |
|
|
8 |
H |
0.215 |
0.547 |
|
|
9 |
H |
0.292 |
0.404 |
|
|
10 |
H |
0.292 |
0.402 |
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.958 |
-1.017 |
0.000 |
1.397 |
CHELPG |
0.327 |
0.626 |
1.153 |
1.352 |
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 |
4.336 |
-0.055 |
-0.088 |
y |
-0.055 |
3.874 |
-0.246 |
z |
-0.088 |
-0.246 |
3.478 |
<r2> (average value of r
2) Å
2
<r2> |
58.968 |
(<r2>)1/2 |
7.679 |
Jump to
S1C1
Energy calculated at HF/3-21G*
| hartrees |
Energy at 0K | -133.503685 |
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/3-21G*
Geometric Data calculated at HF/3-21G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability