Jump to
S1C2
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.185892 |
| Energy at 298.15K | -209.192000 |
| HF Energy | -209.185892 |
| Nuclear repulsion energy | 120.012183 |
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 B1B95/cc-pVTZ
| 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' |
3642 |
3485 |
27.80 |
|
|
|
| 2 |
A' |
3141 |
3006 |
14.58 |
|
|
|
| 3 |
A' |
3048 |
2917 |
52.25 |
|
|
|
| 4 |
A' |
2948 |
2821 |
87.47 |
|
|
|
| 5 |
A' |
1832 |
1753 |
501.13 |
|
|
|
| 6 |
A' |
1539 |
1473 |
21.02 |
|
|
|
| 7 |
A' |
1493 |
1429 |
8.26 |
|
|
|
| 8 |
A' |
1468 |
1405 |
7.71 |
|
|
|
| 9 |
A' |
1402 |
1342 |
13.10 |
|
|
|
| 10 |
A' |
1315 |
1258 |
104.28 |
|
|
|
| 11 |
A' |
1179 |
1128 |
26.21 |
|
|
|
| 12 |
A' |
1020 |
976 |
42.38 |
|
|
|
| 13 |
A' |
619 |
593 |
14.08 |
|
|
|
| 14 |
A' |
346 |
331 |
8.16 |
|
|
|
| 15 |
A" |
3104 |
2971 |
26.47 |
|
|
|
| 16 |
A" |
1485 |
1421 |
5.69 |
|
|
|
| 17 |
A" |
1152 |
1103 |
0.35 |
|
|
|
| 18 |
A" |
1048 |
1003 |
0.98 |
|
|
|
| 19 |
A" |
627 |
600 |
108.70 |
|
|
|
| 20 |
A" |
210 |
201 |
0.49 |
|
|
|
| 21 |
A" |
113 |
108 |
0.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16363.9 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 15661.9 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.285 |
-0.749 |
0.000 |
| O2 |
1.396 |
-1.219 |
0.000 |
| N3 |
0.000 |
0.570 |
0.000 |
| C4 |
-1.329 |
1.116 |
0.000 |
| H5 |
-0.628 |
-1.370 |
0.000 |
| H6 |
0.792 |
1.189 |
0.000 |
| H7 |
-2.041 |
0.295 |
0.000 |
| H8 |
-1.516 |
1.724 |
0.885 |
| H9 |
-1.516 |
1.724 |
-0.885 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2062 | 1.3493 | 2.4669 | 1.1044 | 2.0034 | 2.5504 | 3.1844 | 3.1844 |
O2 | 1.2062 | | 2.2694 | 3.5891 | 2.0298 | 2.4835 | 3.7565 | 4.2335 | 4.2335 | N3 | 1.3493 | 2.2694 | | 1.4369 | 2.0385 | 1.0054 | 2.0598 | 2.1003 | 2.1003 | C4 | 2.4669 | 3.5891 | 1.4369 | | 2.5828 | 2.1218 | 1.0872 | 1.0893 | 1.0893 | H5 | 1.1044 | 2.0298 | 2.0385 | 2.5828 | | 2.9264 | 2.1838 | 3.3374 | 3.3374 | H6 | 2.0034 | 2.4835 | 1.0054 | 2.1218 | 2.9264 | | 2.9708 | 2.5283 | 2.5283 | H7 | 2.5504 | 3.7565 | 2.0598 | 1.0872 | 2.1838 | 2.9708 | | 1.7604 | 1.7604 | H8 | 3.1844 | 4.2335 | 2.1003 | 1.0893 | 3.3374 | 2.5283 | 1.7604 | | 1.7697 | H9 | 3.1844 | 4.2335 | 2.1003 | 1.0893 | 3.3374 | 2.5283 | 1.7604 | 1.7697 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.574 |
|
C1 |
N3 |
H6 |
115.836 |
| O2 |
C1 |
N3 |
125.166 |
|
O2 |
C1 |
H5 |
122.860 |
| N3 |
C1 |
H5 |
111.974 |
|
N3 |
C4 |
H7 |
108.593 |
| N3 |
C4 |
H8 |
111.760 |
|
N3 |
C4 |
H9 |
111.760 |
| C4 |
N3 |
H6 |
119.590 |
|
H7 |
C4 |
H8 |
107.971 |
| H7 |
C4 |
H9 |
107.971 |
|
H8 |
C4 |
H9 |
108.647 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.129 |
|
|
|
| 2 |
O |
-0.337 |
|
|
|
| 3 |
N |
-0.108 |
|
|
|
| 4 |
C |
-0.224 |
|
|
|
| 5 |
H |
0.041 |
|
|
|
| 6 |
H |
0.164 |
|
|
|
| 7 |
H |
0.108 |
|
|
|
| 8 |
H |
0.113 |
|
|
|
| 9 |
H |
0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.035 |
2.786 |
0.000 |
4.120 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.431 |
4.022 |
0.000 |
| y |
4.022 |
-24.260 |
0.000 |
| z |
0.000 |
0.000 |
-24.599 |
|
| Traceless |
| | x | y | z |
| x |
-2.001 |
4.022 |
0.000 |
| y |
4.022 |
1.255 |
0.000 |
| z |
0.000 |
0.000 |
0.746 |
|
| Polar |
| 3z2-r2 | 1.492 |
| x2-y2 | -2.171 |
| xy | 4.022 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.101 |
-1.089 |
0.000 |
| y |
-1.089 |
6.078 |
0.000 |
| z |
0.000 |
0.000 |
3.738 |
<r2> (average value of r
2) Å
2
| <r2> |
88.032 |
| (<r2>)1/2 |
9.383 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.185892 |
| Energy at 298.15K | -209.192000 |
| HF Energy | -209.185892 |
| Nuclear repulsion energy | 120.012183 |
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 B1B95/cc-pVTZ
Geometric Data calculated at B1B95/cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.187593 |
| Energy at 298.15K | -209.193709 |
| HF Energy | -209.187593 |
| Nuclear repulsion energy | 122.201590 |
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 B1B95/cc-pVTZ
| 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 |
3680 |
3522 |
28.30 |
|
|
|
| 2 |
A |
3175 |
3039 |
0.54 |
|
|
|
| 3 |
A |
3114 |
2981 |
26.79 |
|
|
|
| 4 |
A |
3057 |
2926 |
43.95 |
|
|
|
| 5 |
A |
2968 |
2840 |
111.48 |
|
|
|
| 6 |
A |
1819 |
1741 |
347.58 |
|
|
|
| 7 |
A |
1568 |
1500 |
104.38 |
|
|
|
| 8 |
A |
1502 |
1437 |
6.80 |
|
|
|
| 9 |
A |
1496 |
1432 |
30.18 |
|
|
|
| 10 |
A |
1447 |
1385 |
17.07 |
|
|
|
| 11 |
A |
1424 |
1363 |
3.71 |
|
|
|
| 12 |
A |
1236 |
1183 |
73.73 |
|
|
|
| 13 |
A |
1166 |
1116 |
19.82 |
|
|
|
| 14 |
A |
1154 |
1105 |
0.81 |
|
|
|
| 15 |
A |
1031 |
987 |
0.01 |
|
|
|
| 16 |
A |
980 |
938 |
21.17 |
|
|
|
| 17 |
A |
775 |
741 |
0.89 |
|
|
|
| 18 |
A |
545 |
522 |
40.47 |
|
|
|
| 19 |
A |
315 |
301 |
13.59 |
|
|
|
| 20 |
A |
275 |
264 |
65.37 |
|
|
|
| 21 |
A |
84 |
80 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16404.9 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 15701.1 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 B1B95/cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.859 |
0.433 |
0.004 |
| O2 |
1.359 |
-0.670 |
-0.000 |
| N3 |
-0.467 |
0.656 |
-0.020 |
| C4 |
-1.410 |
-0.438 |
0.005 |
| H5 |
1.452 |
1.358 |
0.018 |
| H6 |
-0.794 |
1.599 |
0.057 |
| H7 |
-2.402 |
-0.056 |
-0.212 |
| H8 |
-1.134 |
-1.171 |
-0.747 |
| H9 |
-1.419 |
-0.933 |
0.974 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2109 | 1.3448 | 2.4306 | 1.0989 | 2.0235 | 3.3045 | 2.6662 | 2.8276 |
O2 | 1.2109 | | 2.2568 | 2.7792 | 2.0297 | 3.1284 | 3.8171 | 2.6506 | 2.9555 | N3 | 1.3448 | 2.2568 | | 1.4446 | 2.0442 | 1.0014 | 2.0706 | 2.0764 | 2.1021 | C4 | 2.4306 | 2.7792 | 1.4446 | | 3.3794 | 2.1293 | 1.0850 | 1.0859 | 1.0885 | H5 | 1.0989 | 2.0297 | 2.0442 | 3.3794 | | 2.2594 | 4.1120 | 3.6974 | 3.7955 | H6 | 2.0235 | 3.1284 | 1.0014 | 2.1293 | 2.2594 | | 2.3235 | 2.9049 | 2.7652 | H7 | 3.3045 | 3.8171 | 2.0706 | 1.0850 | 4.1120 | 2.3235 | | 1.7716 | 1.7736 | H8 | 2.6662 | 2.6506 | 2.0764 | 1.0859 | 3.6974 | 2.9049 | 1.7716 | | 1.7607 | H9 | 2.8276 | 2.9555 | 2.1021 | 1.0885 | 3.7955 | 2.7652 | 1.7736 | 1.7607 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.197 |
|
C1 |
N3 |
H6 |
118.444 |
| O2 |
C1 |
N3 |
123.935 |
|
O2 |
C1 |
H5 |
122.901 |
| N3 |
C1 |
H5 |
113.162 |
|
N3 |
C4 |
H7 |
109.054 |
| N3 |
C4 |
H8 |
109.466 |
|
N3 |
C4 |
H9 |
111.395 |
| C4 |
N3 |
H6 |
119.951 |
|
H7 |
C4 |
H8 |
109.388 |
| H7 |
C4 |
H9 |
109.372 |
|
H8 |
C4 |
H9 |
108.139 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.139 |
|
|
|
| 2 |
O |
-0.352 |
|
|
|
| 3 |
N |
-0.133 |
|
|
|
| 4 |
C |
-0.242 |
|
|
|
| 5 |
H |
0.059 |
|
|
|
| 6 |
H |
0.165 |
|
|
|
| 7 |
H |
0.112 |
|
|
|
| 8 |
H |
0.140 |
|
|
|
| 9 |
H |
0.112 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.896 |
2.585 |
0.000 |
3.882 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.504 |
2.593 |
0.000 |
| y |
2.593 |
-22.131 |
0.000 |
| z |
0.000 |
0.000 |
-24.627 |
|
| Traceless |
| | x | y | z |
| x |
-2.125 |
2.593 |
0.000 |
| y |
2.593 |
2.935 |
0.000 |
| z |
0.000 |
0.000 |
-0.810 |
|
| Polar |
| 3z2-r2 | -1.619 |
| x2-y2 | -3.373 |
| xy | 2.593 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.512 |
-0.041 |
0.000 |
| y |
-0.041 |
5.436 |
0.000 |
| z |
0.000 |
0.000 |
3.733 |
<r2> (average value of r
2) Å
2
| <r2> |
77.600 |
| (<r2>)1/2 |
8.809 |