Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -133.930241 |
Energy at 298.15K | -133.935719 |
HF Energy | -133.930241 |
Nuclear repulsion energy | 70.996282 |
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 B3PW91/6-311G*
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' |
3459 |
3330 |
4.39 |
|
|
|
2 |
A' |
3148 |
3030 |
14.92 |
|
|
|
3 |
A' |
3036 |
2922 |
13.18 |
|
|
|
4 |
A' |
2996 |
2884 |
80.10 |
|
|
|
5 |
A' |
1747 |
1682 |
71.35 |
|
|
|
6 |
A' |
1483 |
1427 |
17.60 |
|
|
|
7 |
A' |
1451 |
1397 |
25.81 |
|
|
|
8 |
A' |
1394 |
1342 |
16.53 |
|
|
|
9 |
A' |
1291 |
1242 |
34.11 |
|
|
|
10 |
A' |
1070 |
1030 |
27.98 |
|
|
|
11 |
A' |
932 |
897 |
7.89 |
|
|
|
12 |
A' |
490 |
472 |
17.54 |
|
|
|
13 |
A" |
3091 |
2976 |
18.56 |
|
|
|
14 |
A" |
1488 |
1433 |
12.05 |
|
|
|
15 |
A" |
1136 |
1093 |
9.19 |
|
|
|
16 |
A" |
1083 |
1043 |
12.40 |
|
|
|
17 |
A" |
687 |
661 |
61.35 |
|
|
|
18 |
A" |
198 |
190 |
1.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15089.5 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 14526.6 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.029 |
-0.635 |
0.000 |
C2 |
0.000 |
0.448 |
0.000 |
N3 |
1.240 |
0.187 |
0.000 |
H4 |
-0.545 |
-1.612 |
0.000 |
H5 |
-1.678 |
-0.553 |
0.879 |
H6 |
-1.678 |
-0.553 |
-0.879 |
H7 |
-0.396 |
1.476 |
0.000 |
H8 |
1.787 |
1.050 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.4939 | 2.4137 | 1.0906 | 1.0958 | 1.0958 | 2.2041 | 3.2817 |
C2 | 1.4939 | | 1.2675 | 2.1311 | 2.1422 | 2.1422 | 1.1018 | 1.8858 | N3 | 2.4137 | 1.2675 | | 2.5348 | 3.1362 | 3.1362 | 2.0830 | 1.0213 | H4 | 1.0906 | 2.1311 | 2.5348 | | 1.7831 | 1.7831 | 3.0921 | 3.5391 | H5 | 1.0958 | 2.1422 | 3.1362 | 1.7831 | | 1.7582 | 2.5557 | 3.9175 | H6 | 1.0958 | 2.1422 | 3.1362 | 1.7831 | 1.7582 | | 2.5557 | 3.9175 | H7 | 2.2041 | 1.1018 | 2.0830 | 3.0921 | 2.5557 | 2.5557 | | 2.2244 | H8 | 3.2817 | 1.8858 | 1.0213 | 3.5391 | 3.9175 | 3.9175 | 2.2244 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
121.663 |
|
C1 |
C2 |
H7 |
115.403 |
C2 |
C1 |
H4 |
110.114 |
|
C2 |
C1 |
H5 |
110.691 |
C2 |
C1 |
H6 |
110.691 |
|
C2 |
N3 |
H8 |
110.504 |
N3 |
C2 |
H7 |
122.934 |
|
H4 |
C1 |
H5 |
109.287 |
H4 |
C1 |
H6 |
109.287 |
|
H5 |
C1 |
H6 |
106.697 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.684 |
|
|
|
2 |
C |
-0.017 |
|
|
|
3 |
N |
-0.465 |
|
|
|
4 |
H |
0.244 |
|
|
|
5 |
H |
0.232 |
|
|
|
6 |
H |
0.232 |
|
|
|
7 |
H |
0.176 |
|
|
|
8 |
H |
0.282 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.416 |
1.464 |
0.000 |
2.037 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.664 |
2.567 |
0.000 |
y |
2.567 |
-17.630 |
0.000 |
z |
0.000 |
0.000 |
-19.771 |
|
Traceless |
| x | y | z |
x |
-0.964 |
2.567 |
0.000 |
y |
2.567 |
2.088 |
0.000 |
z |
0.000 |
0.000 |
-1.124 |
|
Polar |
3z2-r2 | -2.247 |
x2-y2 | -2.035 |
xy | 2.567 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.856 |
0.316 |
0.000 |
y |
0.316 |
4.366 |
0.000 |
z |
0.000 |
0.000 |
3.040 |
<r2> (average value of r
2) Å
2
<r2> |
50.186 |
(<r2>)1/2 |
7.084 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -133.928939 |
Energy at 298.15K | -133.934372 |
HF Energy | -133.928939 |
Nuclear repulsion energy | 70.902749 |
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 B3PW91/6-311G*
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' |
3412 |
3285 |
11.71 |
|
|
|
2 |
A' |
3121 |
3005 |
33.91 |
|
|
|
3 |
A' |
3068 |
2954 |
32.63 |
|
|
|
4 |
A' |
3030 |
2917 |
11.51 |
|
|
|
5 |
A' |
1745 |
1680 |
72.06 |
|
|
|
6 |
A' |
1490 |
1435 |
31.96 |
|
|
|
7 |
A' |
1439 |
1386 |
22.06 |
|
|
|
8 |
A' |
1402 |
1349 |
10.74 |
|
|
|
9 |
A' |
1294 |
1246 |
60.35 |
|
|
|
10 |
A' |
1072 |
1032 |
19.67 |
|
|
|
11 |
A' |
913 |
879 |
4.38 |
|
|
|
12 |
A' |
492 |
473 |
7.78 |
|
|
|
13 |
A" |
3093 |
2978 |
14.53 |
|
|
|
14 |
A" |
1483 |
1427 |
12.45 |
|
|
|
15 |
A" |
1157 |
1114 |
53.17 |
|
|
|
16 |
A" |
1080 |
1040 |
9.16 |
|
|
|
17 |
A" |
689 |
663 |
7.79 |
|
|
|
18 |
A" |
168 |
162 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15074.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 14511.9 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.017 |
-0.625 |
0.000 |
C2 |
0.000 |
0.478 |
0.000 |
N3 |
1.263 |
0.385 |
0.000 |
H4 |
-0.547 |
-1.612 |
0.000 |
H5 |
-1.667 |
-0.548 |
0.878 |
H6 |
-1.667 |
-0.548 |
-0.878 |
H7 |
-0.410 |
1.495 |
0.000 |
H8 |
1.549 |
-0.599 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
H4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5000 | 2.4937 | 1.0934 | 1.0956 | 1.0956 | 2.2050 | 2.5655 |
C2 | 1.5000 | | 1.2667 | 2.1609 | 2.1454 | 2.1454 | 1.0967 | 1.8865 | N3 | 2.4937 | 1.2667 | | 2.6959 | 3.1983 | 3.1983 | 2.0083 | 1.0248 | H4 | 1.0934 | 2.1609 | 2.6959 | | 1.7774 | 1.7774 | 3.1105 | 2.3280 | H5 | 1.0956 | 2.1454 | 3.1983 | 1.7774 | | 1.7565 | 2.5542 | 3.3340 | H6 | 1.0956 | 2.1454 | 3.1983 | 1.7774 | 1.7565 | | 2.5542 | 3.3340 | H7 | 2.2050 | 1.0967 | 2.0083 | 3.1105 | 2.5542 | 2.5542 | | 2.8677 | H8 | 2.5655 | 1.8865 | 1.0248 | 2.3280 | 3.3340 | 3.3340 | 2.8677 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
128.459 |
|
C1 |
C2 |
H7 |
115.362 |
C2 |
C1 |
H4 |
111.906 |
|
C2 |
C1 |
H5 |
110.523 |
C2 |
C1 |
H6 |
110.523 |
|
C2 |
N3 |
H8 |
110.381 |
N3 |
C2 |
H7 |
116.178 |
|
H4 |
C1 |
H5 |
108.575 |
H4 |
C1 |
H6 |
108.575 |
|
H5 |
C1 |
H6 |
106.563 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.707 |
|
|
|
2 |
C |
-0.005 |
|
|
|
3 |
N |
-0.466 |
|
|
|
4 |
H |
0.223 |
|
|
|
5 |
H |
0.240 |
|
|
|
6 |
H |
0.240 |
|
|
|
7 |
H |
0.206 |
|
|
|
8 |
H |
0.268 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.014 |
-1.501 |
0.000 |
2.512 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-21.184 |
-3.348 |
0.000 |
y |
-3.348 |
-18.944 |
0.000 |
z |
0.000 |
0.000 |
-19.726 |
|
Traceless |
| x | y | z |
x |
-1.849 |
-3.348 |
0.000 |
y |
-3.348 |
1.512 |
0.000 |
z |
0.000 |
0.000 |
0.338 |
|
Polar |
3z2-r2 | 0.675 |
x2-y2 | -2.240 |
xy | -3.348 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.719 |
-0.034 |
0.000 |
y |
-0.034 |
4.331 |
0.000 |
z |
0.000 |
0.000 |
3.025 |
<r2> (average value of r
2) Å
2
<r2> |
50.349 |
(<r2>)1/2 |
7.096 |