Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -209.101310 |
Energy at 298.15K | -209.107374 |
Nuclear repulsion energy | 117.628563 |
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 |
3829 |
3686 |
64.80 |
|
|
|
2 |
A |
3143 |
3026 |
17.07 |
|
|
|
3 |
A |
3100 |
2984 |
17.60 |
|
|
|
4 |
A |
3036 |
2922 |
22.61 |
|
|
|
5 |
A |
1753 |
1688 |
1.57 |
|
|
|
6 |
A |
1498 |
1442 |
17.09 |
|
|
|
7 |
A |
1467 |
1412 |
16.43 |
|
|
|
8 |
A |
1411 |
1358 |
30.29 |
|
|
|
9 |
A |
1306 |
1258 |
48.80 |
|
|
|
10 |
A |
1160 |
1116 |
3.52 |
|
|
|
11 |
A |
1036 |
998 |
158.01 |
|
|
|
12 |
A |
922 |
888 |
9.74 |
|
|
|
13 |
A |
571 |
550 |
14.70 |
|
|
|
14 |
A |
326 |
314 |
2.87 |
|
|
|
15 |
A |
3089 |
2974 |
19.53 |
|
|
|
16 |
A |
1490 |
1434 |
11.61 |
|
|
|
17 |
A |
1080 |
1040 |
0.49 |
|
|
|
18 |
A |
914 |
880 |
10.85 |
|
|
|
19 |
A |
436 |
420 |
163.67 |
|
|
|
20 |
A |
290 |
279 |
0.59 |
|
|
|
21 |
A |
206 |
198 |
0.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16031.7 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15433.7 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.293 |
1.301 |
0.000 |
C2 |
0.000 |
0.562 |
0.000 |
N3 |
0.009 |
-0.708 |
0.000 |
O4 |
1.307 |
-1.210 |
0.000 |
H5 |
1.174 |
-2.162 |
0.000 |
H6 |
-2.131 |
0.603 |
0.000 |
H7 |
-1.373 |
1.948 |
0.880 |
H8 |
-1.373 |
1.948 |
-0.880 |
H9 |
0.943 |
1.115 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4893 | 2.3937 | 3.6148 | 4.2525 | 1.0909 | 1.0954 | 1.0954 | 2.2441 |
C2 | 1.4893 | | 1.2699 | 2.2020 | 2.9667 | 2.1318 | 2.1406 | 2.1406 | 1.0936 | N3 | 2.3937 | 1.2699 | | 1.3923 | 1.8641 | 2.5097 | 3.1208 | 3.1208 | 2.0486 | O4 | 3.6148 | 2.2020 | 1.3923 | | 0.9614 | 3.8874 | 4.2349 | 4.2349 | 2.3533 | H5 | 4.2525 | 2.9667 | 1.8641 | 0.9614 | | 4.3101 | 4.9156 | 4.9156 | 3.2854 | H6 | 1.0909 | 2.1318 | 2.5097 | 3.8874 | 4.3101 | | 1.7773 | 1.7773 | 3.1171 | H7 | 1.0954 | 2.1406 | 3.1208 | 4.2349 | 4.9156 | 1.7773 | | 1.7603 | 2.6146 | H8 | 1.0954 | 2.1406 | 3.1208 | 4.2349 | 4.9156 | 1.7773 | 1.7603 | | 2.6146 | H9 | 2.2441 | 1.0936 | 2.0486 | 2.3533 | 3.2854 | 3.1171 | 2.6146 | 2.6146 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
120.144 |
|
C1 |
C2 |
H9 |
119.865 |
C2 |
C1 |
H6 |
110.472 |
|
C2 |
C1 |
H7 |
110.910 |
C2 |
C1 |
H8 |
110.910 |
|
C2 |
N3 |
O4 |
111.528 |
N3 |
C2 |
H9 |
119.991 |
|
N3 |
O4 |
H5 |
103.210 |
H6 |
C1 |
H7 |
108.758 |
|
H6 |
C1 |
H8 |
108.758 |
H7 |
C1 |
H8 |
106.927 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.489 |
|
|
|
2 |
H |
0.411 |
|
|
|
3 |
N |
-0.122 |
|
|
|
4 |
C |
-0.008 |
|
|
|
5 |
H |
0.198 |
|
|
|
6 |
C |
-0.701 |
|
|
|
7 |
H |
0.243 |
|
|
|
8 |
H |
0.234 |
|
|
|
9 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.373 |
0.397 |
0.000 |
0.545 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.399 |
-2.222 |
0.000 |
y |
-2.222 |
-18.269 |
0.000 |
z |
0.000 |
0.000 |
-25.097 |
|
Traceless |
| x | y | z |
x |
-3.716 |
-2.222 |
0.000 |
y |
-2.222 |
6.979 |
0.000 |
z |
0.000 |
0.000 |
-3.264 |
|
Polar |
3z2-r2 | -6.527 |
x2-y2 | -7.130 |
xy | -2.222 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
91.297 |
(<r2>)1/2 |
9.555 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -209.100765 |
Energy at 298.15K | -209.106743 |
HF Energy | -209.100765 |
Nuclear repulsion energy | 120.111272 |
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' |
3834 |
3691 |
65.43 |
|
|
|
2 |
A' |
3176 |
3058 |
9.97 |
|
|
|
3 |
A' |
3155 |
3037 |
8.14 |
|
|
|
4 |
A' |
3043 |
2929 |
15.15 |
|
|
|
5 |
A' |
1759 |
1693 |
8.94 |
|
|
|
6 |
A' |
1494 |
1438 |
26.39 |
|
|
|
7 |
A' |
1419 |
1366 |
35.98 |
|
|
|
8 |
A' |
1403 |
1350 |
29.24 |
|
|
|
9 |
A' |
1355 |
1305 |
33.85 |
|
|
|
10 |
A' |
1152 |
1109 |
8.96 |
|
|
|
11 |
A' |
958 |
923 |
152.65 |
|
|
|
12 |
A' |
925 |
891 |
0.33 |
|
|
|
13 |
A' |
683 |
657 |
12.79 |
|
|
|
14 |
A' |
309 |
298 |
1.60 |
|
|
|
15 |
A" |
3094 |
2978 |
16.52 |
|
|
|
16 |
A" |
1499 |
1443 |
13.14 |
|
|
|
17 |
A" |
1067 |
1027 |
0.29 |
|
|
|
18 |
A" |
865 |
833 |
16.32 |
|
|
|
19 |
A" |
518 |
499 |
54.58 |
|
|
|
20 |
A" |
406 |
391 |
97.31 |
|
|
|
21 |
A" |
34 |
32 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16073.9 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15474.4 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 |
-1.445 |
0.488 |
0.000 |
C2 |
0.000 |
0.858 |
0.000 |
N3 |
1.012 |
0.085 |
0.000 |
O4 |
0.659 |
-1.263 |
0.000 |
H5 |
1.512 |
-1.706 |
0.000 |
H6 |
-1.581 |
-0.591 |
0.000 |
H7 |
-1.945 |
0.909 |
0.879 |
H8 |
-1.945 |
0.909 |
-0.879 |
H9 |
0.275 |
1.912 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4920 | 2.4898 | 2.7383 | 3.6830 | 1.0881 | 1.0952 | 1.0952 | 2.2327 |
C2 | 1.4920 | | 1.2728 | 2.2213 | 2.9768 | 2.1444 | 2.1353 | 2.1353 | 1.0889 | N3 | 2.4898 | 1.2728 | | 1.3938 | 1.8601 | 2.6790 | 3.1927 | 3.1927 | 1.9692 | O4 | 2.7383 | 2.2213 | 1.3938 | | 0.9611 | 2.3386 | 3.5034 | 3.5034 | 3.1980 | H5 | 3.6830 | 2.9768 | 1.8601 | 0.9611 | | 3.2877 | 4.4232 | 4.4232 | 3.8234 | H6 | 1.0881 | 2.1444 | 2.6790 | 2.3386 | 3.2877 | | 1.7764 | 1.7764 | 3.1156 | H7 | 1.0952 | 2.1353 | 3.1927 | 3.5034 | 4.4232 | 1.7764 | | 1.7585 | 2.5900 | H8 | 1.0952 | 2.1353 | 3.1927 | 3.5034 | 4.4232 | 1.7764 | 1.7585 | | 2.5900 | H9 | 2.2327 | 1.0889 | 1.9692 | 3.1980 | 3.8234 | 3.1156 | 2.5900 | 2.5900 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
128.285 |
|
C1 |
C2 |
H9 |
118.964 |
C2 |
C1 |
H6 |
111.475 |
|
C2 |
C1 |
H7 |
110.308 |
C2 |
C1 |
H8 |
110.308 |
|
C2 |
N3 |
O4 |
112.737 |
N3 |
C2 |
H9 |
112.750 |
|
N3 |
O4 |
H5 |
102.800 |
H6 |
C1 |
H7 |
108.909 |
|
H6 |
C1 |
H8 |
108.909 |
H7 |
C1 |
H8 |
106.802 |
|
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 |
-0.721 |
|
|
|
2 |
C |
-0.039 |
|
|
|
3 |
N |
-0.114 |
|
|
|
4 |
O |
-0.502 |
|
|
|
5 |
H |
0.416 |
|
|
|
6 |
H |
0.268 |
|
|
|
7 |
H |
0.237 |
|
|
|
8 |
H |
0.237 |
|
|
|
9 |
H |
0.218 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.529 |
0.135 |
0.000 |
0.546 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.719 |
-4.112 |
0.000 |
y |
-4.112 |
-20.918 |
0.000 |
z |
0.000 |
0.000 |
-25.116 |
|
Traceless |
| x | y | z |
x |
0.298 |
-4.112 |
0.000 |
y |
-4.112 |
2.999 |
0.000 |
z |
0.000 |
0.000 |
-3.297 |
|
Polar |
3z2-r2 | -6.594 |
x2-y2 | -1.800 |
xy | -4.112 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.808 |
-1.268 |
0.000 |
y |
-1.268 |
5.925 |
0.000 |
z |
0.000 |
0.000 |
3.261 |
<r2> (average value of r
2) Å
2
<r2> |
78.696 |
(<r2>)1/2 |
8.871 |