Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-311G*
| | hartrees |
| Energy at 0K | -247.101745 |
| Energy at 298.15K | -247.107333 |
| HF Energy | -246.821181 |
| Nuclear repulsion energy | 157.151994 |
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=FULL/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' |
3179 |
3179 |
20.32 |
|
|
|
| 2 |
A' |
3020 |
3020 |
61.16 |
|
|
|
| 3 |
A' |
3011 |
3011 |
24.53 |
|
|
|
| 4 |
A' |
2306 |
2306 |
1.48 |
|
|
|
| 5 |
A' |
1550 |
1550 |
5.58 |
|
|
|
| 6 |
A' |
1531 |
1531 |
9.11 |
|
|
|
| 7 |
A' |
1508 |
1508 |
0.04 |
|
|
|
| 8 |
A' |
1442 |
1442 |
37.45 |
|
|
|
| 9 |
A' |
1246 |
1246 |
36.89 |
|
|
|
| 10 |
A' |
1166 |
1166 |
145.28 |
|
|
|
| 11 |
A' |
1003 |
1003 |
36.84 |
|
|
|
| 12 |
A' |
960 |
960 |
6.20 |
|
|
|
| 13 |
A' |
549 |
549 |
1.46 |
|
|
|
| 14 |
A' |
383 |
383 |
1.86 |
|
|
|
| 15 |
A' |
182 |
182 |
2.17 |
|
|
|
| 16 |
A" |
3073 |
3073 |
56.33 |
|
|
|
| 17 |
A" |
3043 |
3043 |
38.91 |
|
|
|
| 18 |
A" |
1522 |
1522 |
9.99 |
|
|
|
| 19 |
A" |
1289 |
1289 |
3.81 |
|
|
|
| 20 |
A" |
1202 |
1202 |
3.77 |
|
|
|
| 21 |
A" |
1051 |
1051 |
2.38 |
|
|
|
| 22 |
A" |
374 |
374 |
1.39 |
|
|
|
| 23 |
A" |
233 |
233 |
4.64 |
|
|
|
| 24 |
A" |
88 |
88 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17456.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17456.3 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=FULL/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.128 |
-0.361 |
0.000 |
| O2 |
-0.734 |
-0.608 |
0.000 |
| C3 |
0.000 |
0.590 |
0.000 |
| C4 |
1.431 |
0.275 |
0.000 |
| N5 |
2.570 |
0.056 |
0.000 |
| H6 |
-2.616 |
-1.333 |
0.000 |
| H7 |
-2.435 |
0.197 |
0.892 |
| H8 |
-2.435 |
0.197 |
-0.892 |
| H9 |
-0.223 |
1.200 |
-0.886 |
| H10 |
-0.223 |
1.200 |
0.886 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4158 | 2.3312 | 3.6163 | 4.7167 | 1.0869 | 1.0965 | 1.0965 | 2.6177 | 2.6177 |
O2 | 1.4158 | | 1.4052 | 2.3389 | 3.3702 | 2.0160 | 2.0830 | 2.0830 | 2.0775 | 2.0775 | C3 | 2.3312 | 1.4052 | | 1.4658 | 2.6247 | 3.2462 | 2.6232 | 2.6232 | 1.0988 | 1.0988 | C4 | 3.6163 | 2.3389 | 1.4658 | | 1.1592 | 4.3546 | 3.9693 | 3.9693 | 2.0927 | 2.0927 | N5 | 4.7167 | 3.3702 | 2.6247 | 1.1592 | | 5.3680 | 5.0861 | 5.0861 | 3.1458 | 3.1458 | H6 | 1.0869 | 2.0160 | 3.2462 | 4.3546 | 5.3680 | | 1.7804 | 1.7804 | 3.5949 | 3.5949 | H7 | 1.0965 | 2.0830 | 2.6232 | 3.9693 | 5.0861 | 1.7804 | | 1.7842 | 3.0102 | 2.4288 | H8 | 1.0965 | 2.0830 | 2.6232 | 3.9693 | 5.0861 | 1.7804 | 1.7842 | | 2.4288 | 3.0102 | H9 | 2.6177 | 2.0775 | 1.0988 | 2.0927 | 3.1458 | 3.5949 | 3.0102 | 2.4288 | | 1.7722 | H10 | 2.6177 | 2.0775 | 1.0988 | 2.0927 | 3.1458 | 3.5949 | 2.4288 | 3.0102 | 1.7722 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
111.455 |
|
O2 |
C1 |
H6 |
106.581 |
| O2 |
C1 |
H7 |
111.386 |
|
O2 |
C1 |
H8 |
111.386 |
| O2 |
C3 |
C4 |
109.090 |
|
O2 |
C3 |
H9 |
111.547 |
| O2 |
C3 |
H10 |
111.547 |
|
C3 |
C4 |
N5 |
178.482 |
| C4 |
C3 |
H9 |
108.531 |
|
C4 |
C3 |
H10 |
108.531 |
| H6 |
C1 |
H7 |
109.264 |
|
H6 |
C1 |
H8 |
109.264 |
| H7 |
C1 |
H8 |
108.903 |
|
H9 |
C3 |
H10 |
107.500 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-311G*
| | hartrees |
| Energy at 0K | -247.104207 |
| Energy at 298.15K | -247.109896 |
| HF Energy | -246.823172 |
| Nuclear repulsion energy | 159.930025 |
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=FULL/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 |
3180 |
3180 |
21.57 |
|
|
|
| 2 |
A |
3144 |
3144 |
6.35 |
|
|
|
| 3 |
A |
3093 |
3093 |
42.72 |
|
|
|
| 4 |
A |
3033 |
3033 |
43.13 |
|
|
|
| 5 |
A |
3028 |
3028 |
36.46 |
|
|
|
| 6 |
A |
2287 |
2287 |
1.72 |
|
|
|
| 7 |
A |
1543 |
1543 |
11.07 |
|
|
|
| 8 |
A |
1526 |
1526 |
8.43 |
|
|
|
| 9 |
A |
1515 |
1515 |
3.97 |
|
|
|
| 10 |
A |
1504 |
1504 |
1.99 |
|
|
|
| 11 |
A |
1414 |
1414 |
15.28 |
|
|
|
| 12 |
A |
1337 |
1337 |
7.25 |
|
|
|
| 13 |
A |
1239 |
1239 |
30.39 |
|
|
|
| 14 |
A |
1202 |
1202 |
5.86 |
|
|
|
| 15 |
A |
1164 |
1164 |
118.35 |
|
|
|
| 16 |
A |
1049 |
1049 |
7.68 |
|
|
|
| 17 |
A |
951 |
951 |
35.23 |
|
|
|
| 18 |
A |
904 |
904 |
20.83 |
|
|
|
| 19 |
A |
602 |
602 |
1.75 |
|
|
|
| 20 |
A |
399 |
399 |
2.69 |
|
|
|
| 21 |
A |
363 |
363 |
1.05 |
|
|
|
| 22 |
A |
260 |
260 |
10.78 |
|
|
|
| 23 |
A |
180 |
180 |
3.60 |
|
|
|
| 24 |
A |
119 |
119 |
8.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17516.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17516.5 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 B2PLYP=FULL/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.569 |
-0.769 |
0.137 |
| O2 |
1.077 |
0.432 |
-0.440 |
| C3 |
-0.063 |
0.928 |
0.210 |
| C4 |
-1.247 |
0.058 |
0.038 |
| N5 |
-2.162 |
-0.642 |
-0.097 |
| H6 |
2.475 |
-1.022 |
-0.407 |
| H7 |
0.847 |
-1.586 |
0.039 |
| H8 |
1.808 |
-0.626 |
1.197 |
| H9 |
-0.278 |
1.903 |
-0.227 |
| H10 |
0.109 |
1.063 |
1.285 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4203 | 2.3546 | 2.9359 | 3.7397 | 1.0869 | 1.0942 | 1.0962 | 3.2677 | 2.6085 |
O2 | 1.4203 | | 1.4022 | 2.4016 | 3.4293 | 2.0174 | 2.0868 | 2.0820 | 2.0105 | 2.0763 | C3 | 2.3546 | 1.4022 | | 1.4787 | 2.6386 | 3.2588 | 2.6782 | 2.6248 | 1.0897 | 1.0979 | C4 | 2.9359 | 2.4016 | 1.4787 | | 1.1601 | 3.9006 | 2.6619 | 3.3382 | 2.1001 | 2.0985 | N5 | 3.7397 | 3.4293 | 2.6386 | 1.1601 | | 4.6623 | 3.1561 | 4.1756 | 3.1686 | 3.1584 | H6 | 1.0869 | 2.0174 | 3.2588 | 3.9006 | 4.6623 | | 1.7795 | 1.7816 | 4.0202 | 3.5787 | H7 | 1.0942 | 2.0868 | 2.6782 | 2.6619 | 3.1561 | 1.7795 | | 1.7849 | 3.6747 | 3.0188 | H8 | 1.0962 | 2.0820 | 2.6248 | 3.3382 | 4.1756 | 1.7816 | 1.7849 | | 3.5740 | 2.3974 | H9 | 3.2677 | 2.0105 | 1.0897 | 2.1001 | 3.1686 | 4.0202 | 3.6747 | 3.5740 | | 1.7725 | H10 | 2.6085 | 2.0763 | 1.0979 | 2.0985 | 3.1584 | 3.5787 | 3.0188 | 2.3974 | 1.7725 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
113.070 |
|
O2 |
C1 |
H6 |
106.390 |
| O2 |
C1 |
H7 |
111.513 |
|
O2 |
C1 |
H8 |
110.997 |
| O2 |
C3 |
C4 |
112.927 |
|
O2 |
C3 |
H9 |
106.908 |
| O2 |
C3 |
H10 |
111.718 |
|
C3 |
C4 |
N5 |
178.870 |
| C4 |
C3 |
H9 |
108.761 |
|
C4 |
C3 |
H10 |
108.156 |
| H6 |
C1 |
H7 |
109.343 |
|
H6 |
C1 |
H8 |
109.392 |
| H7 |
C1 |
H8 |
109.147 |
|
H9 |
C3 |
H10 |
108.237 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability