Jump to
S1C2
S1C3
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -209.195237 |
| Energy at 298.15K | -209.201211 |
| HF Energy | -209.195237 |
| Nuclear repulsion energy | 118.062091 |
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 BLYP/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' |
3485 |
3472 |
11.11 |
|
|
|
| 2 |
A' |
3030 |
3018 |
18.69 |
|
|
|
| 3 |
A' |
2941 |
2929 |
60.57 |
|
|
|
| 4 |
A' |
2808 |
2797 |
115.03 |
|
|
|
| 5 |
A' |
1728 |
1721 |
393.18 |
|
|
|
| 6 |
A' |
1491 |
1485 |
14.43 |
|
|
|
| 7 |
A' |
1433 |
1428 |
1.13 |
|
|
|
| 8 |
A' |
1425 |
1419 |
7.06 |
|
|
|
| 9 |
A' |
1353 |
1348 |
8.70 |
|
|
|
| 10 |
A' |
1249 |
1244 |
90.73 |
|
|
|
| 11 |
A' |
1110 |
1105 |
39.58 |
|
|
|
| 12 |
A' |
971 |
968 |
43.29 |
|
|
|
| 13 |
A' |
588 |
586 |
12.53 |
|
|
|
| 14 |
A' |
330 |
329 |
7.49 |
|
|
|
| 15 |
A" |
2982 |
2971 |
37.89 |
|
|
|
| 16 |
A" |
1449 |
1443 |
5.65 |
|
|
|
| 17 |
A" |
1112 |
1108 |
0.17 |
|
|
|
| 18 |
A" |
993 |
989 |
1.74 |
|
|
|
| 19 |
A" |
613 |
611 |
107.09 |
|
|
|
| 20 |
A" |
199 |
199 |
0.87 |
|
|
|
| 21 |
A" |
98 |
98 |
0.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15694.7 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 15633.5 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 BLYP/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.287 |
-0.770 |
0.000 |
| O2 |
1.412 |
-1.251 |
0.000 |
| N3 |
0.000 |
0.575 |
0.000 |
| C4 |
-1.344 |
1.153 |
0.000 |
| H5 |
-0.645 |
-1.387 |
0.000 |
| H6 |
0.808 |
1.195 |
0.000 |
| H7 |
-2.077 |
0.335 |
0.000 |
| H8 |
-1.520 |
1.770 |
0.895 |
| H9 |
-1.520 |
1.770 |
-0.895 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2240 | 1.3744 | 2.5211 | 1.1174 | 2.0330 | 2.6095 | 3.2428 | 3.2428 |
O2 | 1.2240 | | 2.3078 | 3.6572 | 2.0615 | 2.5198 | 3.8330 | 4.3041 | 4.3041 | N3 | 1.3744 | 2.3078 | | 1.4633 | 2.0645 | 1.0188 | 2.0909 | 2.1309 | 2.1309 | C4 | 2.5211 | 3.6572 | 1.4633 | | 2.6342 | 2.1522 | 1.0980 | 1.1011 | 1.1011 | H5 | 1.1174 | 2.0615 | 2.0645 | 2.6342 | | 2.9627 | 2.2400 | 3.3961 | 3.3961 | H6 | 2.0330 | 2.5198 | 1.0188 | 2.1522 | 2.9627 | | 3.0104 | 2.5592 | 2.5592 | H7 | 2.6095 | 3.8330 | 2.0909 | 1.0980 | 2.2400 | 3.0104 | | 1.7803 | 1.7803 | H8 | 3.2428 | 4.3041 | 2.1309 | 1.1011 | 3.3961 | 2.5592 | 1.7803 | | 1.7893 | H9 | 3.2428 | 4.3041 | 2.1309 | 1.1011 | 3.3961 | 2.5592 | 1.7803 | 1.7893 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
125.327 |
|
C1 |
N3 |
H6 |
115.509 |
| O2 |
C1 |
N3 |
125.186 |
|
O2 |
C1 |
H5 |
123.332 |
| N3 |
C1 |
H5 |
111.481 |
|
N3 |
C4 |
H7 |
108.599 |
| N3 |
C4 |
H8 |
111.618 |
|
N3 |
C4 |
H9 |
111.618 |
| C4 |
N3 |
H6 |
119.164 |
|
H7 |
C4 |
H8 |
108.100 |
| H7 |
C4 |
H9 |
108.100 |
|
H8 |
C4 |
H9 |
108.684 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.223 |
|
|
|
| 2 |
O |
-0.322 |
|
|
|
| 3 |
N |
-0.333 |
|
|
|
| 4 |
C |
-0.160 |
|
|
|
| 5 |
H |
0.039 |
|
|
|
| 6 |
H |
0.209 |
|
|
|
| 7 |
H |
0.107 |
|
|
|
| 8 |
H |
0.119 |
|
|
|
| 9 |
H |
0.119 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.857 |
2.760 |
0.000 |
3.972 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.466 |
3.732 |
0.000 |
| y |
3.732 |
-24.605 |
0.000 |
| z |
0.000 |
0.000 |
-24.944 |
|
| Traceless |
| | x | y | z |
| x |
-1.691 |
3.732 |
0.000 |
| y |
3.732 |
1.099 |
0.000 |
| z |
0.000 |
0.000 |
0.592 |
|
| Polar |
| 3z2-r2 | 1.184 |
| x2-y2 | -1.860 |
| xy | 3.732 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.091 |
-1.110 |
0.000 |
| y |
-1.110 |
6.195 |
0.000 |
| z |
0.000 |
0.000 |
3.420 |
<r2> (average value of r
2) Å
2
| <r2> |
90.805 |
| (<r2>)1/2 |
9.529 |
Jump to
S1C1
S1C3
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -209.195237 |
| Energy at 298.15K | -209.201211 |
| HF Energy | -209.195237 |
| Nuclear repulsion energy | 118.062091 |
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 BLYP/6-311G**
Geometric Data calculated at BLYP/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at BLYP/6-311G**
| | hartrees |
| Energy at 0K | -209.196980 |
| Energy at 298.15K | -209.202991 |
| HF Energy | -209.196980 |
| Nuclear repulsion energy | 120.216295 |
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 BLYP/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 |
3512 |
3498 |
9.82 |
|
|
|
| 2 |
A |
3064 |
3052 |
2.41 |
|
|
|
| 3 |
A |
2994 |
2982 |
38.18 |
|
|
|
| 4 |
A |
2949 |
2938 |
49.54 |
|
|
|
| 5 |
A |
2823 |
2812 |
148.55 |
|
|
|
| 6 |
A |
1717 |
1710 |
271.95 |
|
|
|
| 7 |
A |
1505 |
1499 |
62.76 |
|
|
|
| 8 |
A |
1467 |
1461 |
6.69 |
|
|
|
| 9 |
A |
1449 |
1443 |
40.22 |
|
|
|
| 10 |
A |
1399 |
1394 |
21.91 |
|
|
|
| 11 |
A |
1375 |
1369 |
3.70 |
|
|
|
| 12 |
A |
1162 |
1157 |
82.84 |
|
|
|
| 13 |
A |
1125 |
1121 |
22.88 |
|
|
|
| 14 |
A |
1116 |
1112 |
0.61 |
|
|
|
| 15 |
A |
970 |
966 |
0.00 |
|
|
|
| 16 |
A |
914 |
911 |
14.65 |
|
|
|
| 17 |
A |
745 |
742 |
0.16 |
|
|
|
| 18 |
A |
531 |
529 |
41.01 |
|
|
|
| 19 |
A |
290 |
288 |
12.68 |
|
|
|
| 20 |
A |
260 |
259 |
64.82 |
|
|
|
| 21 |
A |
95 |
95 |
0.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15729.8 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 15668.5 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 BLYP/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.874 |
0.437 |
0.004 |
| O2 |
1.398 |
-0.676 |
-0.000 |
| N3 |
-0.476 |
0.661 |
-0.019 |
| C4 |
-1.445 |
-0.443 |
0.004 |
| H5 |
1.462 |
1.383 |
0.016 |
| H6 |
-0.808 |
1.618 |
0.055 |
| H7 |
-2.444 |
-0.051 |
-0.220 |
| H8 |
-1.174 |
-1.191 |
-0.751 |
| H9 |
-1.466 |
-0.945 |
0.984 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2297 | 1.3690 | 2.4807 | 1.1136 | 2.0557 | 3.3615 | 2.7232 | 2.8891 |
O2 | 1.2297 | | 2.3018 | 2.8525 | 2.0596 | 3.1825 | 3.8987 | 2.7280 | 3.0405 | N3 | 1.3690 | 2.3018 | | 1.4690 | 2.0685 | 1.0157 | 2.1023 | 2.1100 | 2.1365 | C4 | 2.4807 | 2.8525 | 1.4690 | | 3.4329 | 2.1580 | 1.0964 | 1.0971 | 1.1006 | H5 | 1.1136 | 2.0596 | 2.0685 | 3.4329 | | 2.2820 | 4.1675 | 3.7631 | 3.8639 | H6 | 2.0557 | 3.1825 | 1.0157 | 2.1580 | 2.2820 | | 2.3534 | 2.9455 | 2.8044 | H7 | 3.3615 | 3.8987 | 2.1023 | 1.0964 | 4.1675 | 2.3534 | | 1.7880 | 1.7898 | H8 | 2.7232 | 2.7280 | 2.1100 | 1.0971 | 3.7631 | 2.9455 | 1.7880 | | 1.7759 | H9 | 2.8891 | 3.0405 | 2.1365 | 1.1006 | 3.8639 | 2.8044 | 1.7898 | 1.7759 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.840 |
|
C1 |
N3 |
H6 |
118.342 |
| O2 |
C1 |
N3 |
124.603 |
|
O2 |
C1 |
H5 |
122.943 |
| N3 |
C1 |
H5 |
112.449 |
|
N3 |
C4 |
H7 |
109.205 |
| N3 |
C4 |
H8 |
109.775 |
|
N3 |
C4 |
H9 |
111.695 |
| C4 |
N3 |
H6 |
119.449 |
|
H7 |
C4 |
H8 |
109.205 |
| H7 |
C4 |
H9 |
109.103 |
|
H8 |
C4 |
H9 |
107.816 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.220 |
|
|
|
| 2 |
O |
-0.330 |
|
|
|
| 3 |
N |
-0.341 |
|
|
|
| 4 |
C |
-0.174 |
|
|
|
| 5 |
H |
0.053 |
|
|
|
| 6 |
H |
0.208 |
|
|
|
| 7 |
H |
0.115 |
|
|
|
| 8 |
H |
0.132 |
|
|
|
| 9 |
H |
0.115 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.887 |
2.421 |
0.000 |
3.767 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.722 |
2.381 |
0.000 |
| y |
2.381 |
-22.539 |
0.000 |
| z |
0.000 |
0.000 |
-24.961 |
|
| Traceless |
| | x | y | z |
| x |
-1.972 |
2.381 |
0.000 |
| y |
2.381 |
2.802 |
0.000 |
| z |
0.000 |
0.000 |
-0.831 |
|
| Polar |
| 3z2-r2 | -1.661 |
| x2-y2 | -3.183 |
| xy | 2.381 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.581 |
-0.035 |
0.000 |
| y |
-0.035 |
5.496 |
0.000 |
| z |
0.000 |
0.000 |
3.403 |
<r2> (average value of r
2) Å
2
| <r2> |
80.052 |
| (<r2>)1/2 |
8.947 |