Jump to
S1C2
Energy calculated at SVWN/6-311G*
| hartrees |
Energy at 0K | -208.087719 |
Energy at 298.15K | -208.093772 |
Nuclear repulsion energy | 118.079722 |
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 SVWN/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 |
3692 |
3657 |
85.73 |
|
|
|
2 |
A |
3071 |
3042 |
7.04 |
|
|
|
3 |
A |
3004 |
2976 |
18.34 |
|
|
|
4 |
A |
2962 |
2933 |
15.51 |
|
|
|
5 |
A |
1722 |
1705 |
0.14 |
|
|
|
6 |
A |
1436 |
1422 |
22.33 |
|
|
|
7 |
A |
1412 |
1399 |
8.90 |
|
|
|
8 |
A |
1345 |
1332 |
53.24 |
|
|
|
9 |
A |
1248 |
1236 |
43.95 |
|
|
|
10 |
A |
1136 |
1125 |
2.33 |
|
|
|
11 |
A |
1046 |
1036 |
183.92 |
|
|
|
12 |
A |
905 |
896 |
2.81 |
|
|
|
13 |
A |
568 |
563 |
13.92 |
|
|
|
14 |
A |
321 |
318 |
3.74 |
|
|
|
15 |
A |
3021 |
2992 |
9.06 |
|
|
|
16 |
A |
1420 |
1406 |
15.26 |
|
|
|
17 |
A |
1030 |
1020 |
0.02 |
|
|
|
18 |
A |
878 |
870 |
10.67 |
|
|
|
19 |
A |
461 |
457 |
165.41 |
|
|
|
20 |
A |
288 |
286 |
0.09 |
|
|
|
21 |
A |
215 |
213 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15590.3 cm
-1
Scaled (by 0.9904) Zero Point Vibrational Energy (zpe) 15440.6 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 SVWN/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.282 |
1.290 |
0.000 |
C2 |
0.000 |
0.567 |
0.000 |
N3 |
0.012 |
-0.704 |
0.000 |
O4 |
1.295 |
-1.203 |
0.000 |
H5 |
1.162 |
-2.167 |
0.000 |
H6 |
-2.117 |
0.574 |
0.000 |
H7 |
-1.376 |
1.943 |
0.885 |
H8 |
-1.376 |
1.943 |
-0.885 |
H9 |
0.957 |
1.118 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4719 | 2.3765 | 3.5854 | 4.2335 | 1.0996 | 1.1036 | 1.1036 | 2.2454 |
C2 | 1.4719 | | 1.2706 | 2.1929 | 2.9704 | 2.1173 | 2.1378 | 2.1378 | 1.1041 | N3 | 2.3765 | 1.2706 | | 1.3772 | 1.8613 | 2.4831 | 3.1166 | 3.1166 | 2.0522 | O4 | 3.5854 | 2.1929 | 1.3772 | | 0.9731 | 3.8476 | 4.2207 | 4.2207 | 2.3451 | H5 | 4.2335 | 2.9704 | 1.8613 | 0.9731 | | 4.2744 | 4.9108 | 4.9108 | 3.2909 | H6 | 1.0996 | 2.1173 | 2.4831 | 3.8476 | 4.2744 | | 1.7899 | 1.7899 | 3.1217 | H7 | 1.1036 | 2.1378 | 3.1166 | 4.2207 | 4.9108 | 1.7899 | | 1.7693 | 2.6281 | H8 | 1.1036 | 2.1378 | 3.1166 | 4.2207 | 4.9108 | 1.7899 | 1.7693 | | 2.6281 | H9 | 2.2454 | 1.1041 | 2.0522 | 2.3451 | 3.2909 | 3.1217 | 2.6281 | 2.6281 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
119.941 |
|
C1 |
C2 |
H9 |
120.642 |
C2 |
C1 |
H6 |
110.002 |
|
C2 |
C1 |
H7 |
111.413 |
C2 |
C1 |
H8 |
111.413 |
|
C2 |
N3 |
O4 |
111.762 |
N3 |
C2 |
H9 |
119.416 |
|
N3 |
O4 |
H5 |
103.393 |
H6 |
C1 |
H7 |
108.660 |
|
H6 |
C1 |
H8 |
108.660 |
H7 |
C1 |
H8 |
106.573 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at SVWN/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.768 |
|
|
|
2 |
C |
-0.052 |
|
|
|
3 |
N |
-0.109 |
|
|
|
4 |
O |
-0.462 |
|
|
|
5 |
H |
0.417 |
|
|
|
6 |
H |
0.259 |
|
|
|
7 |
H |
0.255 |
|
|
|
8 |
H |
0.255 |
|
|
|
9 |
H |
0.206 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.255 |
0.180 |
0.000 |
0.312 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.487 |
-2.525 |
0.000 |
y |
-2.525 |
-18.242 |
0.000 |
z |
0.000 |
0.000 |
-25.407 |
|
Traceless |
| x | y | z |
x |
-3.662 |
-2.525 |
0.000 |
y |
-2.525 |
7.206 |
0.000 |
z |
0.000 |
0.000 |
-3.543 |
|
Polar |
3z2-r2 | -7.086 |
x2-y2 | -7.245 |
xy | -2.525 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.646 |
-1.435 |
0.000 |
y |
-1.435 |
7.209 |
0.000 |
z |
0.000 |
0.000 |
3.352 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at SVWN/6-311G*
| hartrees |
Energy at 0K | -208.088316 |
Energy at 298.15K | -208.094290 |
HF Energy | -208.088316 |
Nuclear repulsion energy | 120.818619 |
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 SVWN/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' |
3699 |
3663 |
84.17 |
|
|
|
2 |
A' |
3096 |
3066 |
4.40 |
|
|
|
3 |
A' |
3079 |
3049 |
3.52 |
|
|
|
4 |
A' |
2971 |
2943 |
8.39 |
|
|
|
5 |
A' |
1719 |
1703 |
8.49 |
|
|
|
6 |
A' |
1428 |
1414 |
35.03 |
|
|
|
7 |
A' |
1359 |
1346 |
38.89 |
|
|
|
8 |
A' |
1334 |
1322 |
32.03 |
|
|
|
9 |
A' |
1294 |
1282 |
36.24 |
|
|
|
10 |
A' |
1128 |
1117 |
7.19 |
|
|
|
11 |
A' |
965 |
956 |
142.46 |
|
|
|
12 |
A' |
923 |
914 |
26.42 |
|
|
|
13 |
A' |
676 |
670 |
13.30 |
|
|
|
14 |
A' |
318 |
314 |
1.71 |
|
|
|
15 |
A" |
3029 |
3000 |
6.42 |
|
|
|
16 |
A" |
1431 |
1417 |
16.56 |
|
|
|
17 |
A" |
1017 |
1007 |
0.00 |
|
|
|
18 |
A" |
822 |
814 |
21.60 |
|
|
|
19 |
A" |
530 |
525 |
68.16 |
|
|
|
20 |
A" |
409 |
405 |
83.24 |
|
|
|
21 |
A" |
42 |
42 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15633.8 cm
-1
Scaled (by 0.9904) Zero Point Vibrational Energy (zpe) 15483.7 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 SVWN/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.421 |
0.473 |
0.000 |
C2 |
0.000 |
0.866 |
0.000 |
N3 |
1.007 |
0.084 |
0.000 |
O4 |
0.639 |
-1.247 |
0.000 |
H5 |
1.494 |
-1.710 |
0.000 |
H6 |
-1.519 |
-0.620 |
0.000 |
H7 |
-1.942 |
0.879 |
0.884 |
H8 |
-1.942 |
0.879 |
-0.884 |
H9 |
0.281 |
1.926 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4744 | 2.4589 | 2.6839 | 3.6423 | 1.0980 | 1.1031 | 1.1031 | 2.2382 |
C2 | 1.4744 | | 1.2742 | 2.2072 | 2.9775 | 2.1249 | 2.1339 | 2.1339 | 1.0974 | N3 | 2.4589 | 1.2742 | | 1.3816 | 1.8594 | 2.6221 | 3.1793 | 3.1793 | 1.9796 | O4 | 2.6839 | 2.2072 | 1.3816 | | 0.9726 | 2.2468 | 3.4585 | 3.4585 | 3.1936 | H5 | 3.6423 | 2.9775 | 1.8594 | 0.9726 | | 3.2041 | 4.3921 | 4.3921 | 3.8332 | H6 | 1.0980 | 2.1249 | 2.6221 | 2.2468 | 3.2041 | | 1.7908 | 1.7908 | 3.1186 | H7 | 1.1031 | 2.1339 | 3.1793 | 3.4585 | 4.3921 | 1.7908 | | 1.7675 | 2.6120 | H8 | 1.1031 | 2.1339 | 3.1793 | 3.4585 | 4.3921 | 1.7908 | 1.7675 | | 2.6120 | H9 | 2.2382 | 1.0974 | 1.9796 | 3.1936 | 3.8332 | 3.1186 | 2.6120 | 2.6120 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
126.760 |
|
C1 |
C2 |
H9 |
120.281 |
C2 |
C1 |
H6 |
110.534 |
|
C2 |
C1 |
H7 |
110.949 |
C2 |
C1 |
H8 |
110.949 |
|
C2 |
N3 |
O4 |
112.359 |
N3 |
C2 |
H9 |
112.959 |
|
N3 |
O4 |
H5 |
102.955 |
H6 |
C1 |
H7 |
108.902 |
|
H6 |
C1 |
H8 |
108.902 |
H7 |
C1 |
H8 |
106.487 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at SVWN/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.788 |
|
|
|
2 |
C |
-0.089 |
|
|
|
3 |
N |
-0.100 |
|
|
|
4 |
O |
-0.479 |
|
|
|
5 |
H |
0.423 |
|
|
|
6 |
H |
0.282 |
|
|
|
7 |
H |
0.259 |
|
|
|
8 |
H |
0.259 |
|
|
|
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 |
|
-0.457 |
-0.092 |
0.000 |
0.466 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.991 |
-4.289 |
0.000 |
y |
-4.289 |
-20.861 |
0.000 |
z |
0.000 |
0.000 |
-25.416 |
|
Traceless |
| x | y | z |
x |
0.148 |
-4.289 |
0.000 |
y |
-4.289 |
3.342 |
0.000 |
z |
0.000 |
0.000 |
-3.490 |
|
Polar |
3z2-r2 | -6.979 |
x2-y2 | -2.129 |
xy | -4.289 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.039 |
-1.260 |
0.000 |
y |
-1.260 |
6.087 |
0.000 |
z |
0.000 |
0.000 |
3.356 |
<r2> (average value of r
2) Å
2
<r2> |
77.520 |
(<r2>)1/2 |
8.805 |