Jump to
S1C2
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -133.250242 |
| Energy at 298.15K | -133.255670 |
| HF Energy | -133.250242 |
| Nuclear repulsion energy | 71.133238 |
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 LSDA/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' |
3377 |
3335 |
0.00 |
|
|
|
| 2 |
A' |
3079 |
3041 |
4.53 |
|
|
|
| 3 |
A' |
2964 |
2927 |
3.69 |
|
|
|
| 4 |
A' |
2896 |
2861 |
74.17 |
|
|
|
| 5 |
A' |
1721 |
1699 |
74.00 |
|
|
|
| 6 |
A' |
1389 |
1372 |
29.23 |
|
|
|
| 7 |
A' |
1380 |
1363 |
13.88 |
|
|
|
| 8 |
A' |
1310 |
1294 |
28.56 |
|
|
|
| 9 |
A' |
1220 |
1205 |
40.53 |
|
|
|
| 10 |
A' |
1028 |
1015 |
39.52 |
|
|
|
| 11 |
A' |
916 |
904 |
4.72 |
|
|
|
| 12 |
A' |
479 |
473 |
17.73 |
|
|
|
| 13 |
A" |
3031 |
2994 |
4.70 |
|
|
|
| 14 |
A" |
1398 |
1381 |
15.00 |
|
|
|
| 15 |
A" |
1087 |
1074 |
7.88 |
|
|
|
| 16 |
A" |
1029 |
1016 |
10.69 |
|
|
|
| 17 |
A" |
662 |
654 |
59.93 |
|
|
|
| 18 |
A" |
204 |
201 |
0.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14584.5 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 14405.1 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 LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.027 |
-0.617 |
0.000 |
| C2 |
0.000 |
0.446 |
0.000 |
| N3 |
1.235 |
0.167 |
0.000 |
| H4 |
-0.536 |
-1.600 |
0.000 |
| H5 |
-1.682 |
-0.529 |
0.884 |
| H6 |
-1.682 |
-0.529 |
-0.884 |
| H7 |
-0.391 |
1.487 |
0.000 |
| H8 |
1.804 |
1.026 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4778 | 2.3940 | 1.0989 | 1.1032 | 1.1032 | 2.1975 | 3.2727 |
C2 | 1.4778 | | 1.2666 | 2.1151 | 2.1350 | 2.1350 | 1.1119 | 1.8947 | N3 | 2.3940 | 1.2666 | | 2.5018 | 3.1261 | 3.1261 | 2.0950 | 1.0304 | H4 | 1.0989 | 2.1151 | 2.5018 | | 1.8001 | 1.8001 | 3.0902 | 3.5172 | H5 | 1.1032 | 2.1350 | 3.1261 | 1.8001 | | 1.7672 | 2.5511 | 3.9172 | H6 | 1.1032 | 2.1350 | 3.1261 | 1.8001 | 1.7672 | | 2.5511 | 3.9172 | H7 | 2.1975 | 1.1119 | 2.0950 | 3.0902 | 2.5511 | 2.5511 | | 2.2428 | H8 | 3.2727 | 1.8947 | 1.0304 | 3.5172 | 3.9172 | 3.9172 | 2.2428 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
121.270 |
|
C1 |
C2 |
H7 |
115.385 |
| C2 |
C1 |
H4 |
109.462 |
|
C2 |
C1 |
H5 |
110.790 |
| C2 |
C1 |
H6 |
110.790 |
|
C2 |
N3 |
H8 |
110.731 |
| N3 |
C2 |
H7 |
123.345 |
|
H4 |
C1 |
H5 |
109.657 |
| H4 |
C1 |
H6 |
109.657 |
|
H5 |
C1 |
H6 |
106.438 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.420 |
|
|
|
| 2 |
C |
-0.062 |
|
|
|
| 3 |
N |
-0.312 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
| 6 |
H |
0.164 |
|
|
|
| 7 |
H |
0.111 |
|
|
|
| 8 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.366 |
1.390 |
0.000 |
1.949 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.515 |
2.599 |
0.000 |
| y |
2.599 |
-17.996 |
0.000 |
| z |
0.000 |
0.000 |
-19.904 |
|
| Traceless |
| | x | y | z |
| x |
-0.565 |
2.599 |
0.000 |
| y |
2.599 |
1.713 |
0.000 |
| z |
0.000 |
0.000 |
-1.148 |
|
| Polar |
| 3z2-r2 | -2.297 |
| x2-y2 | -1.519 |
| xy | 2.599 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.141 |
0.351 |
0.000 |
| y |
0.351 |
4.716 |
0.000 |
| z |
0.000 |
0.000 |
3.211 |
<r2> (average value of r
2) Å
2
| <r2> |
49.926 |
| (<r2>)1/2 |
7.066 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -133.249150 |
| Energy at 298.15K | -133.254542 |
| HF Energy | -133.249150 |
| Nuclear repulsion energy | 71.062253 |
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 LSDA/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' |
3311 |
3270 |
5.15 |
|
|
|
| 2 |
A' |
3055 |
3017 |
13.30 |
|
|
|
| 3 |
A' |
2969 |
2932 |
28.55 |
|
|
|
| 4 |
A' |
2957 |
2920 |
4.26 |
|
|
|
| 5 |
A' |
1722 |
1701 |
70.33 |
|
|
|
| 6 |
A' |
1398 |
1381 |
33.25 |
|
|
|
| 7 |
A' |
1368 |
1351 |
27.40 |
|
|
|
| 8 |
A' |
1317 |
1300 |
24.78 |
|
|
|
| 9 |
A' |
1229 |
1213 |
57.77 |
|
|
|
| 10 |
A' |
1039 |
1026 |
20.31 |
|
|
|
| 11 |
A' |
897 |
886 |
8.16 |
|
|
|
| 12 |
A' |
477 |
471 |
7.31 |
|
|
|
| 13 |
A" |
3030 |
2993 |
2.99 |
|
|
|
| 14 |
A" |
1391 |
1374 |
15.93 |
|
|
|
| 15 |
A" |
1107 |
1093 |
49.86 |
|
|
|
| 16 |
A" |
1028 |
1016 |
9.76 |
|
|
|
| 17 |
A" |
669 |
661 |
4.39 |
|
|
|
| 18 |
A" |
178 |
176 |
1.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14570.0 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 14390.8 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 LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.012 |
-0.608 |
0.000 |
| C2 |
0.000 |
0.476 |
0.000 |
| N3 |
1.261 |
0.368 |
0.000 |
| H4 |
-0.537 |
-1.601 |
0.000 |
| H5 |
-1.669 |
-0.527 |
0.882 |
| H6 |
-1.669 |
-0.527 |
-0.882 |
| H7 |
-0.405 |
1.506 |
0.000 |
| H8 |
1.526 |
-0.634 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4827 | 2.4736 | 1.1015 | 1.1033 | 1.1033 | 2.1993 | 2.5379 |
C2 | 1.4827 | | 1.2657 | 2.1457 | 2.1379 | 2.1379 | 1.1068 | 1.8865 | N3 | 2.4736 | 1.2657 | | 2.6666 | 3.1884 | 3.1884 | 2.0176 | 1.0356 | H4 | 1.1015 | 2.1457 | 2.6666 | | 1.7933 | 1.7933 | 3.1104 | 2.2785 | H5 | 1.1033 | 2.1379 | 3.1884 | 1.7933 | | 1.7650 | 2.5516 | 3.3164 | H6 | 1.1033 | 2.1379 | 3.1884 | 1.7933 | 1.7650 | | 2.5516 | 3.3164 | H7 | 2.1993 | 1.1068 | 2.0176 | 3.1104 | 2.5516 | 2.5516 | | 2.8817 | H8 | 2.5379 | 1.8865 | 1.0356 | 2.2785 | 3.3164 | 3.3164 | 2.8817 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.135 |
|
C1 |
C2 |
H7 |
115.513 |
| C2 |
C1 |
H4 |
111.407 |
|
C2 |
C1 |
H5 |
110.668 |
| C2 |
C1 |
H6 |
110.668 |
|
C2 |
N3 |
H8 |
109.713 |
| N3 |
C2 |
H7 |
116.351 |
|
H4 |
C1 |
H5 |
108.853 |
| H4 |
C1 |
H6 |
108.853 |
|
H5 |
C1 |
H6 |
106.231 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.429 |
|
|
|
| 2 |
C |
-0.065 |
|
|
|
| 3 |
N |
-0.303 |
|
|
|
| 4 |
H |
0.144 |
|
|
|
| 5 |
H |
0.171 |
|
|
|
| 6 |
H |
0.171 |
|
|
|
| 7 |
H |
0.143 |
|
|
|
| 8 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.040 |
-1.456 |
0.000 |
2.506 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.251 |
-3.115 |
0.000 |
| y |
-3.115 |
-19.025 |
0.000 |
| z |
0.000 |
0.000 |
-19.862 |
|
| Traceless |
| | x | y | z |
| x |
-1.808 |
-3.115 |
0.000 |
| y |
-3.115 |
1.532 |
0.000 |
| z |
0.000 |
0.000 |
0.276 |
|
| Polar |
| 3z2-r2 | 0.552 |
| x2-y2 | -2.227 |
| xy | -3.115 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.971 |
-0.029 |
0.000 |
| y |
-0.029 |
4.664 |
0.000 |
| z |
0.000 |
0.000 |
3.200 |
<r2> (average value of r
2) Å
2
| <r2> |
50.020 |
| (<r2>)1/2 |
7.072 |