Jump to
S1C2
Energy calculated at B3LYP/6-31G*
| hartrees |
Energy at 0K | -133.952468 |
Energy at 298.15K | -133.957935 |
HF Energy | -133.952468 |
Nuclear repulsion energy | 70.730393 |
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 B3LYP/6-31G*
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' |
3416 |
3281 |
7.76 |
|
|
|
2 |
A' |
3155 |
3030 |
12.61 |
|
|
|
3 |
A' |
3043 |
2922 |
13.45 |
|
|
|
4 |
A' |
3011 |
2891 |
70.57 |
|
|
|
5 |
A' |
1747 |
1678 |
65.85 |
|
|
|
6 |
A' |
1501 |
1441 |
11.35 |
|
|
|
7 |
A' |
1458 |
1400 |
21.65 |
|
|
|
8 |
A' |
1413 |
1357 |
10.37 |
|
|
|
9 |
A' |
1292 |
1240 |
35.38 |
|
|
|
10 |
A' |
1070 |
1028 |
24.86 |
|
|
|
11 |
A' |
931 |
894 |
8.00 |
|
|
|
12 |
A' |
490 |
470 |
16.33 |
|
|
|
13 |
A" |
3093 |
2971 |
18.35 |
|
|
|
14 |
A" |
1508 |
1448 |
8.24 |
|
|
|
15 |
A" |
1133 |
1088 |
8.31 |
|
|
|
16 |
A" |
1089 |
1045 |
11.99 |
|
|
|
17 |
A" |
684 |
657 |
53.71 |
|
|
|
18 |
A" |
198 |
190 |
1.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15116.6 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 14516.5 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 B3LYP/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.033 |
-0.637 |
0.000 |
C2 |
0.000 |
0.451 |
0.000 |
N3 |
1.246 |
0.187 |
0.000 |
H4 |
-0.548 |
-1.616 |
0.000 |
H5 |
-1.682 |
-0.553 |
0.882 |
H6 |
-1.682 |
-0.553 |
-0.882 |
H7 |
-0.400 |
1.478 |
0.000 |
H8 |
1.794 |
1.054 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5009 | 2.4236 | 1.0928 | 1.0980 | 1.0980 | 2.2081 | 3.2945 |
C2 | 1.5009 | | 1.2734 | 2.1387 | 2.1482 | 2.1482 | 1.1021 | 1.8923 | N3 | 2.4236 | 1.2734 | | 2.5432 | 3.1461 | 3.1461 | 2.0919 | 1.0258 | H4 | 1.0928 | 2.1387 | 2.5432 | | 1.7878 | 1.7878 | 3.0978 | 3.5515 | H5 | 1.0980 | 2.1482 | 3.1461 | 1.7878 | | 1.7633 | 2.5582 | 3.9295 | H6 | 1.0980 | 2.1482 | 3.1461 | 1.7878 | 1.7633 | | 2.5582 | 3.9295 | H7 | 2.2081 | 1.1021 | 2.0919 | 3.0978 | 2.5582 | 2.5582 | | 2.2344 | H8 | 3.2945 | 1.8923 | 1.0258 | 3.5515 | 3.9295 | 3.9295 | 2.2344 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
121.539 |
|
C1 |
C2 |
H7 |
115.193 |
C2 |
C1 |
H4 |
110.098 |
|
C2 |
C1 |
H5 |
110.543 |
C2 |
C1 |
H6 |
110.543 |
|
C2 |
N3 |
H8 |
110.306 |
N3 |
C2 |
H7 |
123.269 |
|
H4 |
C1 |
H5 |
109.382 |
H4 |
C1 |
H6 |
109.382 |
|
H5 |
C1 |
H6 |
106.827 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.481 |
|
|
|
2 |
C |
0.089 |
|
|
|
3 |
N |
-0.510 |
|
|
|
4 |
H |
0.178 |
|
|
|
5 |
H |
0.161 |
|
|
|
6 |
H |
0.161 |
|
|
|
7 |
H |
0.116 |
|
|
|
8 |
H |
0.286 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.399 |
1.396 |
0.000 |
1.976 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.498 |
2.503 |
0.000 |
y |
2.503 |
-17.562 |
0.000 |
z |
0.000 |
0.000 |
-19.513 |
|
Traceless |
| x | y | z |
x |
-0.960 |
2.503 |
0.000 |
y |
2.503 |
1.943 |
0.000 |
z |
0.000 |
0.000 |
-0.983 |
|
Polar |
3z2-r2 | -1.966 |
x2-y2 | -1.935 |
xy | 2.503 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.615 |
0.349 |
0.000 |
y |
0.349 |
4.080 |
0.000 |
z |
0.000 |
0.000 |
2.706 |
<r2> (average value of r
2) Å
2
<r2> |
50.363 |
(<r2>)1/2 |
7.097 |
Jump to
S1C1
Energy calculated at B3LYP/6-31G*
| hartrees |
Energy at 0K | -133.951974 |
Energy at 298.15K | -133.957415 |
HF Energy | -133.951974 |
Nuclear repulsion energy | 70.651793 |
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 B3LYP/6-31G*
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' |
3373 |
3239 |
14.17 |
|
|
|
2 |
A' |
3127 |
3002 |
33.08 |
|
|
|
3 |
A' |
3087 |
2964 |
28.31 |
|
|
|
4 |
A' |
3038 |
2917 |
9.86 |
|
|
|
5 |
A' |
1746 |
1677 |
65.47 |
|
|
|
6 |
A' |
1509 |
1449 |
24.08 |
|
|
|
7 |
A' |
1448 |
1390 |
22.80 |
|
|
|
8 |
A' |
1421 |
1365 |
3.89 |
|
|
|
9 |
A' |
1301 |
1249 |
58.78 |
|
|
|
10 |
A' |
1077 |
1035 |
19.02 |
|
|
|
11 |
A' |
914 |
878 |
3.53 |
|
|
|
12 |
A' |
493 |
473 |
7.21 |
|
|
|
13 |
A" |
3096 |
2973 |
14.27 |
|
|
|
14 |
A" |
1501 |
1441 |
7.81 |
|
|
|
15 |
A" |
1156 |
1111 |
41.55 |
|
|
|
16 |
A" |
1087 |
1044 |
11.57 |
|
|
|
17 |
A" |
691 |
663 |
9.81 |
|
|
|
18 |
A" |
177 |
170 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15120.2 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 14519.9 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 B3LYP/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.022 |
-0.627 |
0.000 |
C2 |
0.000 |
0.480 |
0.000 |
N3 |
1.269 |
0.386 |
0.000 |
H4 |
-0.547 |
-1.614 |
0.000 |
H5 |
-1.672 |
-0.549 |
0.881 |
H6 |
-1.672 |
-0.549 |
-0.881 |
H7 |
-0.412 |
1.497 |
0.000 |
H8 |
1.549 |
-0.605 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5066 | 2.5045 | 1.0955 | 1.0979 | 1.0979 | 2.2096 | 2.5701 |
C2 | 1.5066 | | 1.2726 | 2.1646 | 2.1523 | 2.1523 | 1.0970 | 1.8909 | N3 | 2.5045 | 1.2726 | | 2.7010 | 3.2096 | 3.2096 | 2.0154 | 1.0291 | H4 | 1.0955 | 2.1646 | 2.7010 | | 1.7824 | 1.7824 | 3.1140 | 2.3255 | H5 | 1.0979 | 2.1523 | 3.2096 | 1.7824 | | 1.7618 | 2.5594 | 3.3394 | H6 | 1.0979 | 2.1523 | 3.2096 | 1.7824 | 1.7618 | | 2.5594 | 3.3394 | H7 | 2.2096 | 1.0970 | 2.0154 | 3.1140 | 2.5594 | 2.5594 | | 2.8743 | H8 | 2.5701 | 1.8909 | 1.0291 | 2.3255 | 3.3394 | 3.3394 | 2.8743 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
128.424 |
|
C1 |
C2 |
H7 |
115.237 |
C2 |
C1 |
H4 |
111.611 |
|
C2 |
C1 |
H5 |
110.478 |
C2 |
C1 |
H6 |
110.478 |
|
C2 |
N3 |
H8 |
110.022 |
N3 |
C2 |
H7 |
116.339 |
|
H4 |
C1 |
H5 |
108.705 |
H4 |
C1 |
H6 |
108.705 |
|
H5 |
C1 |
H6 |
106.715 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.494 |
|
|
|
2 |
C |
0.087 |
|
|
|
3 |
N |
-0.505 |
|
|
|
4 |
H |
0.154 |
|
|
|
5 |
H |
0.171 |
|
|
|
6 |
H |
0.171 |
|
|
|
7 |
H |
0.140 |
|
|
|
8 |
H |
0.276 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.980 |
-1.458 |
0.000 |
2.459 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-20.990 |
-3.157 |
0.000 |
y |
-3.157 |
-18.864 |
0.000 |
z |
0.000 |
0.000 |
-19.483 |
|
Traceless |
| x | y | z |
x |
-1.816 |
-3.157 |
0.000 |
y |
-3.157 |
1.372 |
0.000 |
z |
0.000 |
0.000 |
0.444 |
|
Polar |
3z2-r2 | 0.889 |
x2-y2 | -2.125 |
xy | -3.157 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.451 |
-0.125 |
0.000 |
y |
-0.125 |
4.107 |
0.000 |
z |
0.000 |
0.000 |
2.698 |
<r2> (average value of r
2) Å
2
<r2> |
50.500 |
(<r2>)1/2 |
7.106 |