Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -247.321622 |
| Energy at 298.15K | -247.327203 |
| HF Energy | -247.321622 |
| Nuclear repulsion energy | 157.117348 |
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/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' |
3141 |
3035 |
21.76 |
|
|
|
| 2 |
A' |
2986 |
2886 |
63.85 |
|
|
|
| 3 |
A' |
2974 |
2874 |
27.11 |
|
|
|
| 4 |
A' |
2373 |
2293 |
0.31 |
|
|
|
| 5 |
A' |
1531 |
1480 |
6.10 |
|
|
|
| 6 |
A' |
1511 |
1460 |
9.27 |
|
|
|
| 7 |
A' |
1492 |
1442 |
0.08 |
|
|
|
| 8 |
A' |
1429 |
1381 |
36.58 |
|
|
|
| 9 |
A' |
1231 |
1190 |
31.69 |
|
|
|
| 10 |
A' |
1150 |
1111 |
156.67 |
|
|
|
| 11 |
A' |
989 |
956 |
36.80 |
|
|
|
| 12 |
A' |
954 |
921 |
5.92 |
|
|
|
| 13 |
A' |
550 |
532 |
1.84 |
|
|
|
| 14 |
A' |
380 |
367 |
1.95 |
|
|
|
| 15 |
A' |
182 |
176 |
2.24 |
|
|
|
| 16 |
A" |
3032 |
2930 |
62.31 |
|
|
|
| 17 |
A" |
2997 |
2896 |
40.27 |
|
|
|
| 18 |
A" |
1505 |
1454 |
9.99 |
|
|
|
| 19 |
A" |
1277 |
1234 |
3.82 |
|
|
|
| 20 |
A" |
1188 |
1148 |
3.48 |
|
|
|
| 21 |
A" |
1040 |
1005 |
2.07 |
|
|
|
| 22 |
A" |
381 |
368 |
1.51 |
|
|
|
| 23 |
A" |
233 |
225 |
4.68 |
|
|
|
| 24 |
A" |
89 |
86 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17307.2 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 16724.0 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.129 |
-0.388 |
0.000 |
| O2 |
-0.730 |
-0.613 |
0.000 |
| C3 |
0.000 |
0.590 |
0.000 |
| C4 |
1.434 |
0.289 |
0.000 |
| N5 |
2.567 |
0.084 |
0.000 |
| H6 |
-2.602 |
-1.368 |
0.000 |
| H7 |
-2.448 |
0.166 |
0.893 |
| H8 |
-2.448 |
0.166 |
-0.893 |
| H9 |
-0.228 |
1.202 |
-0.886 |
| H10 |
-0.228 |
1.202 |
0.886 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4168 | 2.3427 | 3.6263 | 4.7192 | 1.0887 | 1.0985 | 1.0985 | 2.6314 | 2.6314 |
O2 | 1.4168 | | 1.4069 | 2.3442 | 3.3695 | 2.0188 | 2.0869 | 2.0869 | 2.0808 | 2.0808 | C3 | 2.3427 | 1.4069 | | 1.4649 | 2.6160 | 3.2566 | 2.6398 | 2.6398 | 1.1010 | 1.1010 | C4 | 3.6263 | 2.3442 | 1.4649 | | 1.1514 | 4.3629 | 3.9847 | 3.9847 | 2.0930 | 2.0930 | N5 | 4.7192 | 3.3695 | 2.6160 | 1.1514 | | 5.3689 | 5.0939 | 5.0939 | 3.1380 | 3.1380 | H6 | 1.0887 | 2.0188 | 3.2566 | 4.3629 | 5.3689 | | 1.7823 | 1.7823 | 3.6091 | 3.6091 | H7 | 1.0985 | 2.0869 | 2.6398 | 3.9847 | 5.0939 | 1.7823 | | 1.7867 | 3.0275 | 2.4491 | H8 | 1.0985 | 2.0869 | 2.6398 | 3.9847 | 5.0939 | 1.7823 | 1.7867 | | 2.4491 | 3.0275 | H9 | 2.6314 | 2.0808 | 1.1010 | 2.0930 | 3.1380 | 3.6091 | 3.0275 | 2.4491 | | 1.7728 | H10 | 2.6314 | 2.0808 | 1.1010 | 2.0930 | 3.1380 | 3.6091 | 2.4491 | 3.0275 | 1.7728 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
112.125 |
|
O2 |
C1 |
H6 |
106.632 |
| O2 |
C1 |
H7 |
111.505 |
|
O2 |
C1 |
H8 |
111.505 |
| O2 |
C3 |
C4 |
109.413 |
|
O2 |
C3 |
H9 |
111.557 |
| O2 |
C3 |
H10 |
111.557 |
|
C3 |
C4 |
N5 |
178.424 |
| C4 |
C3 |
H9 |
108.483 |
|
C4 |
C3 |
H10 |
108.483 |
| H6 |
C1 |
H7 |
109.149 |
|
H6 |
C1 |
H8 |
109.149 |
| H7 |
C1 |
H8 |
108.838 |
|
H9 |
C3 |
H10 |
107.241 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.429 |
|
|
|
| 2 |
O |
-0.322 |
|
|
|
| 3 |
C |
-0.199 |
|
|
|
| 4 |
C |
0.088 |
|
|
|
| 5 |
N |
-0.219 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
| 7 |
H |
0.198 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
| 9 |
H |
0.227 |
|
|
|
| 10 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.361 |
1.722 |
0.000 |
4.689 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.257 |
0.680 |
0.000 |
| y |
0.680 |
-29.361 |
0.000 |
| z |
0.000 |
0.000 |
-29.362 |
|
| Traceless |
| | x | y | z |
| x |
-6.895 |
0.680 |
0.000 |
| y |
0.680 |
3.448 |
0.000 |
| z |
0.000 |
0.000 |
3.447 |
|
| Polar |
| 3z2-r2 | 6.893 |
| x2-y2 | -6.895 |
| xy | 0.680 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.225 |
0.049 |
0.000 |
| y |
0.049 |
4.900 |
0.000 |
| z |
0.000 |
0.000 |
4.589 |
<r2> (average value of r
2) Å
2
| <r2> |
143.062 |
| (<r2>)1/2 |
11.961 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -247.323859 |
| Energy at 298.15K | -247.329510 |
| HF Energy | -247.323859 |
| Nuclear repulsion energy | 159.726880 |
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/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 |
3142 |
3036 |
23.04 |
|
|
|
| 2 |
A |
3104 |
2999 |
6.91 |
|
|
|
| 3 |
A |
3055 |
2952 |
45.25 |
|
|
|
| 4 |
A |
2998 |
2897 |
54.91 |
|
|
|
| 5 |
A |
2993 |
2892 |
30.29 |
|
|
|
| 6 |
A |
2355 |
2276 |
0.08 |
|
|
|
| 7 |
A |
1524 |
1473 |
10.89 |
|
|
|
| 8 |
A |
1507 |
1456 |
8.15 |
|
|
|
| 9 |
A |
1496 |
1446 |
3.66 |
|
|
|
| 10 |
A |
1484 |
1434 |
3.43 |
|
|
|
| 11 |
A |
1402 |
1355 |
14.50 |
|
|
|
| 12 |
A |
1324 |
1279 |
7.71 |
|
|
|
| 13 |
A |
1225 |
1184 |
24.49 |
|
|
|
| 14 |
A |
1188 |
1148 |
4.54 |
|
|
|
| 15 |
A |
1146 |
1107 |
126.99 |
|
|
|
| 16 |
A |
1038 |
1003 |
8.28 |
|
|
|
| 17 |
A |
937 |
906 |
35.75 |
|
|
|
| 18 |
A |
896 |
866 |
20.25 |
|
|
|
| 19 |
A |
601 |
581 |
1.73 |
|
|
|
| 20 |
A |
392 |
379 |
2.43 |
|
|
|
| 21 |
A |
367 |
355 |
1.31 |
|
|
|
| 22 |
A |
255 |
246 |
11.31 |
|
|
|
| 23 |
A |
175 |
169 |
3.07 |
|
|
|
| 24 |
A |
115 |
111 |
8.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17359.2 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 16774.2 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 B3LYP/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.596 |
-0.755 |
0.137 |
| O2 |
1.070 |
0.433 |
-0.441 |
| C3 |
-0.076 |
0.919 |
0.209 |
| C4 |
-1.257 |
0.048 |
0.039 |
| N5 |
-2.168 |
-0.644 |
-0.096 |
| H6 |
2.498 |
-0.996 |
-0.424 |
| H7 |
0.889 |
-1.589 |
0.060 |
| H8 |
1.856 |
-0.600 |
1.192 |
| H9 |
-0.295 |
1.896 |
-0.225 |
| H10 |
0.095 |
1.058 |
1.287 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4220 | 2.3672 | 2.9662 | 3.7734 | 1.0886 | 1.0959 | 1.0979 | 3.2766 | 2.6199 |
O2 | 1.4220 | | 1.4043 | 2.4072 | 3.4302 | 2.0201 | 2.0907 | 2.0861 | 2.0125 | 2.0799 | C3 | 2.3672 | 1.4043 | | 1.4776 | 2.6297 | 3.2698 | 2.6912 | 2.6469 | 1.0916 | 1.0998 | C4 | 2.9662 | 2.4072 | 1.4776 | | 1.1523 | 3.9250 | 2.6998 | 3.3831 | 2.0998 | 2.0996 | N5 | 3.7734 | 3.4302 | 2.6297 | 1.1523 | | 4.6906 | 3.2038 | 4.2258 | 3.1589 | 3.1520 | H6 | 1.0886 | 2.0201 | 3.2698 | 3.9250 | 4.6906 | | 1.7811 | 1.7834 | 4.0253 | 3.5943 | H7 | 1.0959 | 2.0907 | 2.6912 | 2.6998 | 3.2038 | 1.7811 | | 1.7874 | 3.6915 | 3.0238 | H8 | 1.0979 | 2.0861 | 2.6469 | 3.3831 | 4.2258 | 1.7834 | 1.7874 | | 3.5872 | 2.4207 | H9 | 3.2766 | 2.0125 | 1.0916 | 2.0998 | 3.1589 | 4.0253 | 3.6915 | 3.5872 | | 1.7724 | H10 | 2.6199 | 2.0799 | 1.0998 | 2.0996 | 3.1520 | 3.5943 | 3.0238 | 2.4207 | 1.7724 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
113.772 |
|
O2 |
C1 |
H6 |
106.393 |
| O2 |
C1 |
H7 |
111.610 |
|
O2 |
C1 |
H8 |
111.110 |
| O2 |
C3 |
C4 |
113.271 |
|
O2 |
C3 |
H9 |
106.810 |
| O2 |
C3 |
H10 |
111.742 |
|
C3 |
C4 |
N5 |
179.133 |
| C4 |
C3 |
H9 |
108.699 |
|
C4 |
C3 |
H10 |
108.202 |
| H6 |
C1 |
H7 |
109.237 |
|
H6 |
C1 |
H8 |
109.302 |
| H7 |
C1 |
H8 |
109.124 |
|
H9 |
C3 |
H10 |
107.949 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.437 |
|
|
|
| 2 |
O |
-0.314 |
|
|
|
| 3 |
C |
-0.241 |
|
|
|
| 4 |
C |
0.088 |
|
|
|
| 5 |
N |
-0.226 |
|
|
|
| 6 |
H |
0.226 |
|
|
|
| 7 |
H |
0.220 |
|
|
|
| 8 |
H |
0.195 |
|
|
|
| 9 |
H |
0.257 |
|
|
|
| 10 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.552 |
1.232 |
1.428 |
3.174 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
4.385 |
1.773 |
0.000 |
4.730 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.307 |
-5.625 |
0.606 |
| y |
-5.625 |
-28.251 |
0.586 |
| z |
0.606 |
0.586 |
-29.906 |
|
| Traceless |
| | x | y | z |
| x |
-7.229 |
-5.625 |
0.606 |
| y |
-5.625 |
4.855 |
0.586 |
| z |
0.606 |
0.586 |
2.374 |
|
| Polar |
| 3z2-r2 | 4.748 |
| x2-y2 | -8.056 |
| xy | -5.625 |
| xz | 0.606 |
| yz | 0.586 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.032 |
0.429 |
0.171 |
| y |
0.429 |
5.677 |
0.226 |
| z |
0.171 |
0.226 |
4.602 |
<r2> (average value of r
2) Å
2
| <r2> |
123.930 |
| (<r2>)1/2 |
11.132 |