Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -247.215351 |
| Energy at 298.15K | -247.220802 |
| HF Energy | -247.215351 |
| Nuclear repulsion energy | 154.116497 |
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 B3LYP/LANL2DZ
| 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' |
3184 |
3061 |
21.69 |
|
|
|
| 2 |
A' |
3012 |
2895 |
70.80 |
|
|
|
| 3 |
A' |
3006 |
2890 |
34.29 |
|
|
|
| 4 |
A' |
2297 |
2208 |
0.33 |
|
|
|
| 5 |
A' |
1519 |
1461 |
9.67 |
|
|
|
| 6 |
A' |
1504 |
1446 |
7.78 |
|
|
|
| 7 |
A' |
1484 |
1427 |
0.37 |
|
|
|
| 8 |
A' |
1417 |
1362 |
20.95 |
|
|
|
| 9 |
A' |
1192 |
1146 |
11.36 |
|
|
|
| 10 |
A' |
1100 |
1057 |
125.81 |
|
|
|
| 11 |
A' |
959 |
922 |
1.44 |
|
|
|
| 12 |
A' |
908 |
872 |
30.71 |
|
|
|
| 13 |
A' |
536 |
515 |
0.76 |
|
|
|
| 14 |
A' |
361 |
347 |
2.15 |
|
|
|
| 15 |
A' |
177 |
170 |
0.83 |
|
|
|
| 16 |
A" |
3087 |
2967 |
66.65 |
|
|
|
| 17 |
A" |
3054 |
2935 |
36.51 |
|
|
|
| 18 |
A" |
1508 |
1450 |
14.81 |
|
|
|
| 19 |
A" |
1250 |
1201 |
1.10 |
|
|
|
| 20 |
A" |
1150 |
1105 |
0.89 |
|
|
|
| 21 |
A" |
1029 |
990 |
2.13 |
|
|
|
| 22 |
A" |
377 |
362 |
0.04 |
|
|
|
| 23 |
A" |
220 |
212 |
6.69 |
|
|
|
| 24 |
A" |
79 |
76 |
1.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17205.2 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 16537.6 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.172 |
-0.455 |
0.000 |
| O2 |
-0.723 |
-0.640 |
0.000 |
| C3 |
0.000 |
0.620 |
0.000 |
| C4 |
1.445 |
0.336 |
0.000 |
| N5 |
2.607 |
0.137 |
0.000 |
| H6 |
-2.597 |
-1.460 |
0.000 |
| H7 |
-2.506 |
0.087 |
0.899 |
| H8 |
-2.506 |
0.087 |
-0.899 |
| H9 |
-0.244 |
1.220 |
-0.893 |
| H10 |
-0.244 |
1.220 |
0.893 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4601 | 2.4231 | 3.7017 | 4.8152 | 1.0918 | 1.1013 | 1.1013 | 2.7049 | 2.7049 |
O2 | 1.4601 | | 1.4526 | 2.3772 | 3.4197 | 2.0456 | 2.1247 | 2.1247 | 2.1177 | 2.1177 | C3 | 2.4231 | 1.4526 | | 1.4723 | 2.6513 | 3.3276 | 2.7154 | 2.7154 | 1.1033 | 1.1033 | C4 | 3.7017 | 2.3772 | 1.4723 | | 1.1792 | 4.4228 | 4.0594 | 4.0594 | 2.1052 | 2.1052 | N5 | 4.8152 | 3.4197 | 2.6513 | 1.1792 | | 5.4438 | 5.1918 | 5.1918 | 3.1779 | 3.1779 | H6 | 1.0918 | 2.0456 | 3.3276 | 4.4228 | 5.4438 | | 1.7914 | 1.7914 | 3.6764 | 3.6764 | H7 | 1.1013 | 2.1247 | 2.7154 | 4.0594 | 5.1918 | 1.7914 | | 1.7974 | 3.1002 | 2.5298 | H8 | 1.1013 | 2.1247 | 2.7154 | 4.0594 | 5.1918 | 1.7914 | 1.7974 | | 2.5298 | 3.1002 | H9 | 2.7049 | 2.1177 | 1.1033 | 2.1052 | 3.1779 | 3.6764 | 3.1002 | 2.5298 | | 1.7867 | H10 | 2.7049 | 2.1177 | 1.1033 | 2.1052 | 3.1779 | 3.6764 | 2.5298 | 3.1002 | 1.7867 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
112.589 |
|
O2 |
C1 |
H6 |
105.661 |
| O2 |
C1 |
H7 |
111.322 |
|
O2 |
C1 |
H8 |
111.322 |
| O2 |
C3 |
C4 |
108.726 |
|
O2 |
C3 |
H9 |
111.165 |
| O2 |
C3 |
H10 |
111.165 |
|
C3 |
C4 |
N5 |
178.552 |
| C4 |
C3 |
H9 |
108.794 |
|
C4 |
C3 |
H10 |
108.794 |
| H6 |
C1 |
H7 |
109.542 |
|
H6 |
C1 |
H8 |
109.542 |
| H7 |
C1 |
H8 |
109.378 |
|
H9 |
C3 |
H10 |
108.139 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.445 |
|
|
|
| 2 |
O |
-0.300 |
|
|
|
| 3 |
C |
-0.211 |
|
|
|
| 4 |
C |
-0.108 |
|
|
|
| 5 |
N |
-0.011 |
|
|
|
| 6 |
H |
0.239 |
|
|
|
| 7 |
H |
0.198 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
| 9 |
H |
0.220 |
|
|
|
| 10 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.815 |
2.217 |
0.000 |
5.301 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.634 |
0.512 |
0.000 |
| y |
0.512 |
-29.309 |
0.000 |
| z |
0.000 |
0.000 |
-29.080 |
|
| Traceless |
| | x | y | z |
| x |
-6.440 |
0.512 |
0.000 |
| y |
0.512 |
3.048 |
0.000 |
| z |
0.000 |
0.000 |
3.392 |
|
| Polar |
| 3z2-r2 | 6.784 |
| x2-y2 | -6.325 |
| xy | 0.512 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.071 |
0.154 |
0.000 |
| y |
0.154 |
4.511 |
0.000 |
| z |
0.000 |
0.000 |
4.070 |
<r2> (average value of r
2) Å
2
| <r2> |
147.542 |
| (<r2>)1/2 |
12.147 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -247.218735 |
| Energy at 298.15K | -247.224289 |
| HF Energy | -247.218735 |
| Nuclear repulsion energy | 156.762503 |
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 B3LYP/LANL2DZ
| 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 |
3185 |
3061 |
22.77 |
|
|
|
| 2 |
A |
3148 |
3026 |
6.27 |
|
|
|
| 3 |
A |
3105 |
2985 |
52.97 |
|
|
|
| 4 |
A |
3035 |
2917 |
41.22 |
|
|
|
| 5 |
A |
3021 |
2903 |
49.14 |
|
|
|
| 6 |
A |
2277 |
2188 |
0.02 |
|
|
|
| 7 |
A |
1519 |
1460 |
15.18 |
|
|
|
| 8 |
A |
1507 |
1449 |
13.74 |
|
|
|
| 9 |
A |
1489 |
1431 |
7.46 |
|
|
|
| 10 |
A |
1482 |
1425 |
3.76 |
|
|
|
| 11 |
A |
1393 |
1339 |
5.77 |
|
|
|
| 12 |
A |
1294 |
1244 |
4.31 |
|
|
|
| 13 |
A |
1194 |
1147 |
8.36 |
|
|
|
| 14 |
A |
1153 |
1109 |
2.11 |
|
|
|
| 15 |
A |
1104 |
1062 |
99.49 |
|
|
|
| 16 |
A |
1026 |
987 |
10.15 |
|
|
|
| 17 |
A |
909 |
874 |
35.26 |
|
|
|
| 18 |
A |
859 |
826 |
18.26 |
|
|
|
| 19 |
A |
588 |
565 |
2.08 |
|
|
|
| 20 |
A |
375 |
361 |
3.13 |
|
|
|
| 21 |
A |
362 |
348 |
2.97 |
|
|
|
| 22 |
A |
245 |
235 |
14.94 |
|
|
|
| 23 |
A |
175 |
168 |
2.90 |
|
|
|
| 24 |
A |
113 |
108 |
11.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17278.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 16608.1 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 B3LYP/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.624 |
-0.784 |
0.136 |
| O2 |
1.101 |
0.460 |
-0.429 |
| C3 |
-0.101 |
0.949 |
0.211 |
| C4 |
-1.270 |
0.048 |
0.036 |
| N5 |
-2.195 |
-0.672 |
-0.099 |
| H6 |
2.551 |
-0.985 |
-0.404 |
| H7 |
0.921 |
-1.616 |
-0.014 |
| H8 |
1.836 |
-0.671 |
1.211 |
| H9 |
-0.318 |
1.913 |
-0.258 |
| H10 |
0.053 |
1.106 |
1.291 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4634 | 2.4465 | 3.0125 | 3.8273 | 1.0919 | 1.0990 | 1.1009 | 3.3470 | 2.7155 |
O2 | 1.4634 | | 1.4470 | 2.4504 | 3.5000 | 2.0470 | 2.1242 | 2.1234 | 2.0380 | 2.1152 | C3 | 2.4465 | 1.4470 | | 1.4853 | 2.6654 | 3.3394 | 2.7698 | 2.7161 | 1.0942 | 1.1022 | C4 | 3.0125 | 2.4504 | 1.4853 | | 1.1801 | 3.9820 | 2.7512 | 3.3974 | 2.1145 | 2.1077 | N5 | 3.8273 | 3.5000 | 2.6654 | 1.1801 | | 4.7656 | 3.2564 | 4.2381 | 3.1987 | 3.1850 | H6 | 1.0919 | 2.0470 | 3.3394 | 3.9820 | 4.7656 | | 1.7909 | 1.7939 | 4.0802 | 3.6722 | H7 | 1.0990 | 2.1242 | 2.7698 | 2.7512 | 3.2564 | 1.7909 | | 1.7973 | 3.7479 | 3.1408 | H8 | 1.1009 | 2.1234 | 2.7161 | 3.3974 | 4.2381 | 1.7939 | 1.7973 | | 3.6709 | 2.5189 | H9 | 3.3470 | 2.0380 | 1.0942 | 2.1145 | 3.1987 | 4.0802 | 3.7479 | 3.6709 | | 1.7858 | H10 | 2.7155 | 2.1152 | 1.1022 | 2.1077 | 3.1850 | 3.6722 | 3.1408 | 2.5189 | 1.7858 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
114.408 |
|
O2 |
C1 |
H6 |
105.542 |
| O2 |
C1 |
H7 |
111.192 |
|
O2 |
C1 |
H8 |
111.014 |
| O2 |
C3 |
C4 |
113.357 |
|
O2 |
C3 |
H9 |
105.800 |
| O2 |
C3 |
H10 |
111.427 |
|
C3 |
C4 |
N5 |
179.661 |
| C4 |
C3 |
H9 |
109.176 |
|
C4 |
C3 |
H10 |
108.181 |
| H6 |
C1 |
H7 |
109.656 |
|
H6 |
C1 |
H8 |
109.789 |
| H7 |
C1 |
H8 |
109.572 |
|
H9 |
C3 |
H10 |
108.791 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.456 |
|
|
|
| 2 |
O |
-0.288 |
|
|
|
| 3 |
C |
-0.243 |
|
|
|
| 4 |
C |
-0.124 |
|
|
|
| 5 |
N |
-0.015 |
|
|
|
| 6 |
H |
0.236 |
|
|
|
| 7 |
H |
0.223 |
|
|
|
| 8 |
H |
0.196 |
|
|
|
| 9 |
H |
0.255 |
|
|
|
| 10 |
H |
0.217 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.390 |
1.023 |
1.837 |
3.183 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.697 |
-6.734 |
1.050 |
| y |
-6.734 |
-28.038 |
0.823 |
| z |
1.050 |
0.823 |
-29.819 |
|
| Traceless |
| | x | y | z |
| x |
-7.769 |
-6.734 |
1.050 |
| y |
-6.734 |
5.221 |
0.823 |
| z |
1.050 |
0.823 |
2.548 |
|
| Polar |
| 3z2-r2 | 5.096 |
| x2-y2 | -8.660 |
| xy | -6.734 |
| xz | 1.050 |
| yz | 0.823 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.874 |
0.574 |
0.124 |
| y |
0.574 |
5.372 |
0.188 |
| z |
0.124 |
0.188 |
4.141 |
<r2> (average value of r
2) Å
2
| <r2> |
127.641 |
| (<r2>)1/2 |
11.298 |