Jump to
S1C2
S1C3
Energy calculated at B2PLYP=FULLultrafine/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.071070 |
| Energy at 298.15K | |
| HF Energy | -224.854023 |
| Nuclear repulsion energy | 123.241939 |
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=FULLultrafine/cc-pVDZ
| 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 |
3684 |
3530 |
27.32 |
63.31 |
0.74 |
0.85 |
| 2 |
A |
3568 |
3419 |
1.51 |
188.19 |
0.08 |
0.15 |
| 3 |
A |
1836 |
1759 |
343.36 |
6.43 |
0.19 |
0.32 |
| 4 |
A |
1620 |
1552 |
0.04 |
5.05 |
0.72 |
0.83 |
| 5 |
A |
1193 |
1143 |
4.87 |
7.75 |
0.30 |
0.46 |
| 6 |
A |
957 |
917 |
6.81 |
10.96 |
0.12 |
0.22 |
| 7 |
A |
651 |
624 |
104.84 |
5.42 |
0.50 |
0.66 |
| 8 |
A |
474 |
455 |
0.57 |
0.73 |
0.71 |
0.83 |
| 9 |
A |
397 |
381 |
69.07 |
1.98 |
0.75 |
0.86 |
| 10 |
B |
3684 |
3530 |
25.04 |
50.53 |
0.75 |
0.86 |
| 11 |
B |
3565 |
3416 |
35.90 |
15.76 |
0.75 |
0.86 |
| 12 |
B |
1628 |
1560 |
168.76 |
3.98 |
0.75 |
0.86 |
| 13 |
B |
1426 |
1367 |
178.83 |
0.82 |
0.75 |
0.86 |
| 14 |
B |
1070 |
1025 |
25.97 |
1.94 |
0.75 |
0.86 |
| 15 |
B |
800 |
766 |
112.35 |
0.04 |
0.75 |
0.86 |
| 16 |
B |
591 |
566 |
192.87 |
3.24 |
0.75 |
0.86 |
| 17 |
B |
557 |
534 |
93.73 |
0.02 |
0.75 |
0.86 |
| 18 |
B |
445 |
426 |
38.45 |
2.84 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 14073.2 cm
-1
Scaled (by 0.9582) Zero Point Vibrational Energy (zpe) 13485.0 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=FULLultrafine/cc-pVDZ
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.147 |
| O2 |
0.000 |
0.000 |
1.367 |
| N3 |
0.000 |
1.163 |
-0.621 |
| N4 |
0.000 |
-1.163 |
-0.621 |
| H5 |
0.255 |
1.974 |
-0.067 |
| H6 |
0.515 |
1.107 |
-1.494 |
| H7 |
-0.255 |
-1.974 |
-0.067 |
| H8 |
-0.515 |
-1.107 |
-1.494 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2193 | 1.3936 | 1.3936 | 2.0024 | 2.0458 | 2.0024 | 2.0458 |
O2 | 1.2193 | | 2.3026 | 2.3026 | 2.4536 | 3.1104 | 2.4536 | 3.1104 | N3 | 1.3936 | 2.3026 | | 2.3255 | 1.0150 | 1.0153 | 3.1958 | 2.4859 | N4 | 1.3936 | 2.3026 | 2.3255 | | 3.1958 | 2.4859 | 1.0150 | 1.0153 | H5 | 2.0024 | 2.4536 | 1.0150 | 3.1958 | | 1.6899 | 3.9818 | 3.4819 | H6 | 2.0458 | 3.1104 | 1.0153 | 2.4859 | 1.6899 | | 3.4819 | 2.4416 | H7 | 2.0024 | 2.4536 | 3.1958 | 1.0150 | 3.9818 | 3.4819 | | 1.6899 | H8 | 2.0458 | 3.1104 | 2.4859 | 1.0153 | 3.4819 | 2.4416 | 1.6899 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
111.513 |
|
C1 |
N3 |
H6 |
115.366 |
| C1 |
N4 |
H7 |
111.513 |
|
C1 |
N4 |
H8 |
115.366 |
| O2 |
C1 |
N3 |
123.451 |
|
O2 |
C1 |
N4 |
123.451 |
| N3 |
C1 |
N4 |
113.098 |
|
H5 |
N3 |
H6 |
112.684 |
| H7 |
N4 |
H8 |
112.684 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.163 |
|
|
|
| 2 |
O |
-0.280 |
|
|
|
| 3 |
N |
-0.154 |
|
|
|
| 4 |
N |
-0.154 |
|
|
|
| 5 |
H |
0.111 |
|
|
|
| 6 |
H |
0.102 |
|
|
|
| 7 |
H |
0.111 |
|
|
|
| 8 |
H |
0.102 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-3.341 |
3.341 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.005 |
3.538 |
0.000 |
| y |
3.538 |
-18.235 |
0.000 |
| z |
0.000 |
0.000 |
-24.914 |
|
| Traceless |
| | x | y | z |
| x |
-2.431 |
3.538 |
0.000 |
| y |
3.538 |
6.224 |
0.000 |
| z |
0.000 |
0.000 |
-3.793 |
|
| Polar |
| 3z2-r2 | -7.587 |
| x2-y2 | -5.770 |
| xy | 3.538 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.280 |
0.252 |
0.000 |
| y |
0.252 |
4.714 |
0.000 |
| z |
0.000 |
0.000 |
4.801 |
<r2> (average value of r
2) Å
2
| <r2> |
68.756 |
| (<r2>)1/2 |
8.292 |
Jump to
S1C1
S1C3
Energy calculated at B2PLYP=FULLultrafine/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.071070 |
| Energy at 298.15K | |
| HF Energy | -224.854023 |
| Nuclear repulsion energy | 123.241939 |
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=FULLultrafine/cc-pVDZ
Geometric Data calculated at B2PLYP=FULLultrafine/cc-pVDZ
Point Group is C2
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP=FULLultrafine/cc-pVDZ
| | hartrees |
| Energy at 0K | -225.066929 |
| Energy at 298.15K | |
| HF Energy | -224.850934 |
| Nuclear repulsion energy | 123.502457 |
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=FULLultrafine/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3782 |
3624 |
50.59 |
|
|
|
| 2 |
A1 |
3639 |
3487 |
6.24 |
|
|
|
| 3 |
A1 |
1820 |
1744 |
415.51 |
|
|
|
| 4 |
A1 |
1605 |
1538 |
2.51 |
|
|
|
| 5 |
A1 |
1141 |
1093 |
0.49 |
|
|
|
| 6 |
A1 |
981 |
940 |
8.48 |
|
|
|
| 7 |
A1 |
478 |
458 |
2.50 |
|
|
|
| 8 |
A2 |
375 |
359 |
0.00 |
|
|
|
| 9 |
A2 |
466i |
447i |
0.00 |
|
|
|
| 10 |
B1 |
774 |
742 |
6.36 |
|
|
|
| 11 |
B1 |
571 |
547 |
9.66 |
|
|
|
| 12 |
B1 |
381i |
366i |
434.08 |
|
|
|
| 13 |
B2 |
3780 |
3622 |
43.54 |
|
|
|
| 14 |
B2 |
3630 |
3478 |
63.57 |
|
|
|
| 15 |
B2 |
1612 |
1545 |
299.82 |
|
|
|
| 16 |
B2 |
1434 |
1374 |
168.52 |
|
|
|
| 17 |
B2 |
988 |
947 |
12.61 |
|
|
|
| 18 |
B2 |
564 |
540 |
14.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13162.4 cm
-1
Scaled (by 0.9582) Zero Point Vibrational Energy (zpe) 12612.2 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=FULLultrafine/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.145 |
| O2 |
0.000 |
0.000 |
1.368 |
| N3 |
0.000 |
1.158 |
-0.601 |
| N4 |
0.000 |
-1.158 |
-0.601 |
| H5 |
0.000 |
2.028 |
-0.091 |
| H6 |
0.000 |
1.178 |
-1.609 |
| H7 |
0.000 |
-2.028 |
-0.091 |
| H8 |
0.000 |
-1.178 |
-1.609 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2231 | 1.3773 | 1.3773 | 2.0419 | 2.1121 | 2.0419 | 2.1121 |
O2 | 1.2231 | | 2.2839 | 2.2839 | 2.4983 | 3.2009 | 2.4983 | 3.2009 | N3 | 1.3773 | 2.2839 | | 2.3162 | 1.0086 | 1.0079 | 3.2269 | 2.5441 | N4 | 1.3773 | 2.2839 | 2.3162 | | 3.2269 | 2.5441 | 1.0086 | 1.0079 | H5 | 2.0419 | 2.4983 | 1.0086 | 3.2269 | | 1.7397 | 4.0565 | 3.5473 | H6 | 2.1121 | 3.2009 | 1.0079 | 2.5441 | 1.7397 | | 3.5473 | 2.3559 | H7 | 2.0419 | 2.4983 | 3.2269 | 1.0086 | 4.0565 | 3.5473 | | 1.7397 | H8 | 2.1121 | 3.2009 | 2.5441 | 1.0079 | 3.5473 | 2.3559 | 1.7397 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.859 |
|
C1 |
N3 |
H6 |
123.897 |
| C1 |
N4 |
H7 |
116.859 |
|
C1 |
N4 |
H8 |
123.897 |
| O2 |
C1 |
N3 |
122.768 |
|
O2 |
C1 |
N4 |
122.768 |
| N3 |
C1 |
N4 |
114.463 |
|
H5 |
N3 |
H6 |
119.244 |
| H7 |
N4 |
H8 |
119.244 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability