Jump to
S1C2
S1C3
Energy calculated at B2PLYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.116316 |
| Energy at 298.15K | -209.122375 |
| HF Energy | -208.861829 |
| Nuclear repulsion energy | 119.407321 |
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 B2PLYP/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' |
3624 |
3476 |
28.86 |
|
|
|
| 2 |
A' |
3141 |
3014 |
14.69 |
|
|
|
| 3 |
A' |
3050 |
2926 |
51.77 |
|
|
|
| 4 |
A' |
2962 |
2842 |
83.62 |
|
|
|
| 5 |
A' |
1786 |
1714 |
449.21 |
|
|
|
| 6 |
A' |
1547 |
1484 |
14.22 |
|
|
|
| 7 |
A' |
1489 |
1428 |
5.04 |
|
|
|
| 8 |
A' |
1478 |
1418 |
9.04 |
|
|
|
| 9 |
A' |
1406 |
1349 |
12.59 |
|
|
|
| 10 |
A' |
1310 |
1257 |
109.61 |
|
|
|
| 11 |
A' |
1171 |
1123 |
33.08 |
|
|
|
| 12 |
A' |
1016 |
975 |
41.29 |
|
|
|
| 13 |
A' |
613 |
588 |
12.75 |
|
|
|
| 14 |
A' |
345 |
331 |
7.78 |
|
|
|
| 15 |
A" |
3106 |
2980 |
26.47 |
|
|
|
| 16 |
A" |
1501 |
1440 |
5.32 |
|
|
|
| 17 |
A" |
1162 |
1115 |
0.48 |
|
|
|
| 18 |
A" |
1046 |
1003 |
1.61 |
|
|
|
| 19 |
A" |
617 |
592 |
108.34 |
|
|
|
| 20 |
A" |
201 |
193 |
0.64 |
|
|
|
| 21 |
A" |
99 |
95 |
0.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16333.9 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15670.8 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 B2PLYP/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.284 |
-0.755 |
0.000 |
| O2 |
1.403 |
-1.229 |
0.000 |
| N3 |
0.000 |
0.571 |
0.000 |
| C4 |
-1.335 |
1.127 |
0.000 |
| H5 |
-0.628 |
-1.374 |
0.000 |
| H6 |
0.795 |
1.189 |
0.000 |
| H7 |
-2.053 |
0.310 |
0.000 |
| H8 |
-1.516 |
1.736 |
0.886 |
| H9 |
-1.516 |
1.736 |
-0.886 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2145 | 1.3565 | 2.4831 | 1.1030 | 2.0103 | 2.5684 | 3.1983 | 3.1983 |
O2 | 1.2145 | | 2.2824 | 3.6121 | 2.0358 | 2.4936 | 3.7826 | 4.2535 | 4.2535 | N3 | 1.3565 | 2.2824 | | 1.4461 | 2.0448 | 1.0073 | 2.0692 | 2.1066 | 2.1066 | C4 | 2.4831 | 3.6121 | 1.4461 | | 2.5998 | 2.1313 | 1.0875 | 1.0895 | 1.0895 | H5 | 1.1030 | 2.0358 | 2.0448 | 2.5998 | | 2.9325 | 2.2063 | 3.3536 | 3.3536 | H6 | 2.0103 | 2.4936 | 1.0073 | 2.1313 | 2.9325 | | 2.9806 | 2.5346 | 2.5346 | H7 | 2.5684 | 3.7826 | 2.0692 | 1.0875 | 2.2063 | 2.9806 | | 1.7620 | 1.7620 | H8 | 3.1983 | 4.2535 | 2.1066 | 1.0895 | 3.3536 | 2.5346 | 1.7620 | | 1.7710 | H9 | 3.1983 | 4.2535 | 2.1066 | 1.0895 | 3.3536 | 2.5346 | 1.7620 | 1.7710 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
124.714 |
|
C1 |
N3 |
H6 |
115.738 |
| O2 |
C1 |
N3 |
125.092 |
|
O2 |
C1 |
H5 |
122.838 |
| N3 |
C1 |
H5 |
112.070 |
|
N3 |
C4 |
H7 |
108.682 |
| N3 |
C4 |
H8 |
111.584 |
|
N3 |
C4 |
H9 |
111.584 |
| C4 |
N3 |
H6 |
119.548 |
|
H7 |
C4 |
H8 |
108.069 |
| H7 |
C4 |
H9 |
108.069 |
|
H8 |
C4 |
H9 |
108.730 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.122 |
|
|
|
| 2 |
O |
-0.325 |
|
|
|
| 3 |
N |
-0.119 |
|
|
|
| 4 |
C |
-0.198 |
|
|
|
| 5 |
H |
0.041 |
|
|
|
| 6 |
H |
0.161 |
|
|
|
| 7 |
H |
0.104 |
|
|
|
| 8 |
H |
0.107 |
|
|
|
| 9 |
H |
0.107 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.054 |
2.776 |
0.000 |
4.127 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.695 |
4.012 |
0.000 |
| y |
4.012 |
-24.556 |
0.000 |
| z |
0.000 |
0.000 |
-24.899 |
|
| Traceless |
| | x | y | z |
| x |
-1.968 |
4.012 |
0.000 |
| y |
4.012 |
1.241 |
0.000 |
| z |
0.000 |
0.000 |
0.727 |
|
| Polar |
| 3z2-r2 | 1.454 |
| x2-y2 | -2.139 |
| xy | 4.012 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.138 |
-1.119 |
0.000 |
| y |
-1.119 |
6.143 |
0.000 |
| z |
0.000 |
0.000 |
3.742 |
<r2> (average value of r
2) Å
2
| <r2> |
89.018 |
| (<r2>)1/2 |
9.435 |
Jump to
S1C1
S1C3
Energy calculated at B2PLYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.116316 |
| Energy at 298.15K | -209.122375 |
| HF Energy | -208.861829 |
| Nuclear repulsion energy | 119.407321 |
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 B2PLYP/cc-pVTZ
Geometric Data calculated at B2PLYP/cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -209.118048 |
| Energy at 298.15K | -209.124074 |
| HF Energy | -208.863348 |
| Nuclear repulsion energy | 121.552035 |
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 B2PLYP/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 |
3660 |
3511 |
27.73 |
|
|
|
| 2 |
A |
3172 |
3043 |
0.71 |
|
|
|
| 3 |
A |
3114 |
2988 |
26.90 |
|
|
|
| 4 |
A |
3057 |
2933 |
43.50 |
|
|
|
| 5 |
A |
2977 |
2856 |
109.67 |
|
|
|
| 6 |
A |
1775 |
1703 |
309.16 |
|
|
|
| 7 |
A |
1566 |
1503 |
85.47 |
|
|
|
| 8 |
A |
1518 |
1456 |
6.24 |
|
|
|
| 9 |
A |
1507 |
1446 |
38.84 |
|
|
|
| 10 |
A |
1452 |
1393 |
19.87 |
|
|
|
| 11 |
A |
1427 |
1369 |
6.16 |
|
|
|
| 12 |
A |
1227 |
1177 |
82.95 |
|
|
|
| 13 |
A |
1168 |
1120 |
18.23 |
|
|
|
| 14 |
A |
1165 |
1118 |
1.07 |
|
|
|
| 15 |
A |
1028 |
987 |
0.01 |
|
|
|
| 16 |
A |
963 |
923 |
18.14 |
|
|
|
| 17 |
A |
770 |
738 |
0.65 |
|
|
|
| 18 |
A |
537 |
516 |
38.11 |
|
|
|
| 19 |
A |
298 |
286 |
13.36 |
|
|
|
| 20 |
A |
259 |
248 |
69.14 |
|
|
|
| 21 |
A |
63 |
60 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16351.2 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15687.3 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 B2PLYP/cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.863 |
0.436 |
0.004 |
| O2 |
1.374 |
-0.671 |
-0.000 |
| N3 |
-0.471 |
0.657 |
-0.020 |
| C4 |
-1.422 |
-0.441 |
0.005 |
| H5 |
1.451 |
1.364 |
0.019 |
| H6 |
-0.797 |
1.603 |
0.058 |
| H7 |
-2.414 |
-0.054 |
-0.210 |
| H8 |
-1.151 |
-1.175 |
-0.749 |
| H9 |
-1.432 |
-0.938 |
0.974 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.2191 | 1.3526 | 2.4475 | 1.0993 | 2.0302 | 3.3199 | 2.6867 | 2.8452 |
O2 | 1.2191 | | 2.2736 | 2.8058 | 2.0369 | 3.1447 | 3.8435 | 2.6819 | 2.9823 | N3 | 1.3526 | 2.2736 | | 1.4528 | 2.0486 | 1.0035 | 2.0773 | 2.0858 | 2.1110 | C4 | 2.4475 | 2.8058 | 1.4528 | | 3.3933 | 2.1377 | 1.0858 | 1.0864 | 1.0892 | H5 | 1.0993 | 2.0369 | 2.0486 | 3.3933 | | 2.2614 | 4.1232 | 3.7163 | 3.8112 | H6 | 2.0302 | 3.1447 | 1.0035 | 2.1377 | 2.2614 | | 2.3302 | 2.9145 | 2.7743 | H7 | 3.3199 | 3.8435 | 2.0773 | 1.0858 | 4.1232 | 2.3302 | | 1.7722 | 1.7740 | H8 | 2.6867 | 2.6819 | 2.0858 | 1.0864 | 3.7163 | 2.9145 | 1.7722 | | 1.7613 | H9 | 2.8452 | 2.9823 | 2.1110 | 1.0892 | 3.8112 | 2.7743 | 1.7740 | 1.7613 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
C4 |
121.443 |
|
C1 |
N3 |
H6 |
118.262 |
| O2 |
C1 |
N3 |
124.205 |
|
O2 |
C1 |
H5 |
122.860 |
| N3 |
C1 |
H5 |
112.934 |
|
N3 |
C4 |
H7 |
108.970 |
| N3 |
C4 |
H8 |
109.612 |
|
N3 |
C4 |
H9 |
111.489 |
| C4 |
N3 |
H6 |
119.875 |
|
H7 |
C4 |
H8 |
109.341 |
| H7 |
C4 |
H9 |
109.301 |
|
H8 |
C4 |
H9 |
108.100 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.132 |
|
|
|
| 2 |
O |
-0.340 |
|
|
|
| 3 |
N |
-0.143 |
|
|
|
| 4 |
C |
-0.215 |
|
|
|
| 5 |
H |
0.058 |
|
|
|
| 6 |
H |
0.162 |
|
|
|
| 7 |
H |
0.106 |
|
|
|
| 8 |
H |
0.134 |
|
|
|
| 9 |
H |
0.106 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.907 |
2.558 |
-0.000 |
3.872 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.807 |
2.605 |
0.000 |
| y |
2.605 |
-22.427 |
-0.001 |
| z |
0.000 |
-0.001 |
-24.924 |
|
| Traceless |
| | x | y | z |
| x |
-2.131 |
2.605 |
0.000 |
| y |
2.605 |
2.938 |
-0.001 |
| z |
0.000 |
-0.001 |
-0.807 |
|
| Polar |
| 3z2-r2 | -1.613 |
| x2-y2 | -3.379 |
| xy | 2.605 |
| xz | 0.000 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.576 |
-0.088 |
0.000 |
| y |
-0.088 |
5.490 |
0.000 |
| z |
0.000 |
0.000 |
3.738 |
<r2> (average value of r
2) Å
2
| <r2> |
78.546 |
| (<r2>)1/2 |
8.863 |