Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -247.163722 |
| Energy at 298.15K | -247.169289 |
| HF Energy | -247.163722 |
| Nuclear repulsion energy | 157.493863 |
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 B1B95/6-31+G**
| 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' |
3187 |
3049 |
13.99 |
|
|
|
| 2 |
A' |
3023 |
2891 |
60.52 |
|
|
|
| 3 |
A' |
3012 |
2881 |
25.05 |
|
|
|
| 4 |
A' |
2408 |
2304 |
0.77 |
|
|
|
| 5 |
A' |
1517 |
1451 |
6.66 |
|
|
|
| 6 |
A' |
1496 |
1431 |
8.76 |
|
|
|
| 7 |
A' |
1480 |
1416 |
0.30 |
|
|
|
| 8 |
A' |
1414 |
1352 |
39.35 |
|
|
|
| 9 |
A' |
1238 |
1184 |
91.39 |
|
|
|
| 10 |
A' |
1187 |
1135 |
99.59 |
|
|
|
| 11 |
A' |
1021 |
977 |
36.07 |
|
|
|
| 12 |
A' |
962 |
921 |
7.92 |
|
|
|
| 13 |
A' |
549 |
525 |
1.28 |
|
|
|
| 14 |
A' |
376 |
360 |
1.81 |
|
|
|
| 15 |
A' |
180 |
173 |
2.24 |
|
|
|
| 16 |
A" |
3085 |
2951 |
43.21 |
|
|
|
| 17 |
A" |
3047 |
2915 |
26.90 |
|
|
|
| 18 |
A" |
1496 |
1431 |
10.80 |
|
|
|
| 19 |
A" |
1266 |
1211 |
3.95 |
|
|
|
| 20 |
A" |
1183 |
1132 |
3.28 |
|
|
|
| 21 |
A" |
1026 |
982 |
1.84 |
|
|
|
| 22 |
A" |
374 |
358 |
1.31 |
|
|
|
| 23 |
A" |
228 |
218 |
4.94 |
|
|
|
| 24 |
A" |
89 |
85 |
0.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17422.3 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 16666.2 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.124 |
-0.362 |
0.000 |
| O2 |
-0.736 |
-0.607 |
0.000 |
| C3 |
0.000 |
0.582 |
0.000 |
| C4 |
1.430 |
0.272 |
0.000 |
| N5 |
2.567 |
0.065 |
0.000 |
| H6 |
-2.614 |
-1.333 |
0.000 |
| H7 |
-2.431 |
0.196 |
0.893 |
| H8 |
-2.431 |
0.196 |
-0.893 |
| H9 |
-0.219 |
1.194 |
-0.887 |
| H10 |
-0.219 |
1.194 |
0.887 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4096 | 2.3245 | 3.6098 | 4.7110 | 1.0881 | 1.0973 | 1.0973 | 2.6145 | 2.6145 |
O2 | 1.4096 | | 1.3984 | 2.3371 | 3.3712 | 2.0136 | 2.0778 | 2.0778 | 2.0729 | 2.0729 | C3 | 2.3245 | 1.3984 | | 1.4628 | 2.6189 | 3.2408 | 2.6187 | 2.6187 | 1.0997 | 1.0997 | C4 | 3.6098 | 2.3371 | 1.4628 | | 1.1564 | 4.3506 | 3.9635 | 3.9635 | 2.0871 | 2.0871 | N5 | 4.7110 | 3.3712 | 2.6189 | 1.1564 | | 5.3670 | 5.0796 | 5.0796 | 3.1347 | 3.1347 | H6 | 1.0881 | 2.0136 | 3.2408 | 4.3506 | 5.3670 | | 1.7810 | 1.7810 | 3.5929 | 3.5929 | H7 | 1.0973 | 2.0778 | 2.6187 | 3.9635 | 5.0796 | 1.7810 | | 1.7865 | 3.0096 | 2.4264 | H8 | 1.0973 | 2.0778 | 2.6187 | 3.9635 | 5.0796 | 1.7810 | 1.7865 | | 2.4264 | 3.0096 | H9 | 2.6145 | 2.0729 | 1.0997 | 2.0871 | 3.1347 | 3.5929 | 3.0096 | 2.4264 | | 1.7744 | H10 | 2.6145 | 2.0729 | 1.0997 | 2.0871 | 3.1347 | 3.5929 | 2.4264 | 3.0096 | 1.7744 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
111.745 |
|
O2 |
C1 |
H6 |
106.745 |
| O2 |
C1 |
H7 |
111.353 |
|
O2 |
C1 |
H8 |
111.353 |
| O2 |
C3 |
C4 |
109.515 |
|
O2 |
C3 |
H9 |
111.590 |
| O2 |
C3 |
H10 |
111.590 |
|
C3 |
C4 |
N5 |
178.031 |
| C4 |
C3 |
H9 |
108.232 |
|
C4 |
C3 |
H10 |
108.232 |
| H6 |
C1 |
H7 |
109.168 |
|
H6 |
C1 |
H8 |
109.168 |
| H7 |
C1 |
H8 |
108.994 |
|
H9 |
C3 |
H10 |
107.558 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.203 |
|
|
|
| 2 |
O |
-0.314 |
|
|
|
| 3 |
C |
0.015 |
|
|
|
| 4 |
C |
0.158 |
|
|
|
| 5 |
N |
-0.469 |
|
|
|
| 6 |
H |
0.173 |
|
|
|
| 7 |
H |
0.142 |
|
|
|
| 8 |
H |
0.142 |
|
|
|
| 9 |
H |
0.178 |
|
|
|
| 10 |
H |
0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.543 |
1.891 |
0.000 |
4.921 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.434 |
0.668 |
0.000 |
| y |
0.668 |
-29.573 |
0.000 |
| z |
0.000 |
0.000 |
-29.410 |
|
| Traceless |
| | x | y | z |
| x |
-6.942 |
0.668 |
0.000 |
| y |
0.668 |
3.349 |
0.000 |
| z |
0.000 |
0.000 |
3.593 |
|
| Polar |
| 3z2-r2 | 7.186 |
| x2-y2 | -6.861 |
| xy | 0.668 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.758 |
-0.040 |
0.000 |
| y |
-0.040 |
5.297 |
0.000 |
| z |
0.000 |
0.000 |
4.979 |
<r2> (average value of r
2) Å
2
| <r2> |
142.542 |
| (<r2>)1/2 |
11.939 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -247.169924 |
| Energy at 298.15K | -247.175508 |
| HF Energy | -247.169924 |
| Nuclear repulsion energy | 160.187986 |
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 B1B95/6-31+G**
| 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 |
3041 |
14.58 |
|
|
|
| 2 |
A |
3134 |
2998 |
3.10 |
|
|
|
| 3 |
A |
3091 |
2957 |
32.70 |
|
|
|
| 4 |
A |
3021 |
2890 |
45.53 |
|
|
|
| 5 |
A |
3018 |
2887 |
28.63 |
|
|
|
| 6 |
A |
2376 |
2273 |
0.20 |
|
|
|
| 7 |
A |
1505 |
1440 |
11.26 |
|
|
|
| 8 |
A |
1486 |
1421 |
11.16 |
|
|
|
| 9 |
A |
1472 |
1408 |
0.77 |
|
|
|
| 10 |
A |
1464 |
1400 |
4.68 |
|
|
|
| 11 |
A |
1382 |
1322 |
15.59 |
|
|
|
| 12 |
A |
1308 |
1251 |
9.50 |
|
|
|
| 13 |
A |
1221 |
1168 |
87.64 |
|
|
|
| 14 |
A |
1172 |
1121 |
61.33 |
|
|
|
| 15 |
A |
1170 |
1119 |
11.77 |
|
|
|
| 16 |
A |
1024 |
980 |
9.49 |
|
|
|
| 17 |
A |
961 |
919 |
33.76 |
|
|
|
| 18 |
A |
906 |
867 |
18.10 |
|
|
|
| 19 |
A |
600 |
574 |
1.84 |
|
|
|
| 20 |
A |
382 |
366 |
2.50 |
|
|
|
| 21 |
A |
353 |
338 |
1.81 |
|
|
|
| 22 |
A |
243 |
233 |
11.85 |
|
|
|
| 23 |
A |
163 |
156 |
2.58 |
|
|
|
| 24 |
A |
110 |
105 |
10.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17370.6 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 16616.7 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 B1B95/6-31+G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.562 |
-0.770 |
0.134 |
| O2 |
1.079 |
0.434 |
-0.431 |
| C3 |
-0.062 |
0.928 |
0.205 |
| C4 |
-1.241 |
0.056 |
0.035 |
| N5 |
-2.158 |
-0.640 |
-0.095 |
| H6 |
2.468 |
-1.027 |
-0.412 |
| H7 |
0.833 |
-1.582 |
0.029 |
| H8 |
1.804 |
-0.638 |
1.197 |
| H9 |
-0.284 |
1.901 |
-0.238 |
| H10 |
0.100 |
1.070 |
1.284 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4156 | 2.3515 | 2.9242 | 3.7300 | 1.0890 | 1.0964 | 1.0978 | 3.2687 | 2.6168 |
O2 | 1.4156 | | 1.3971 | 2.3968 | 3.4280 | 2.0164 | 2.0829 | 2.0794 | 2.0117 | 2.0747 | C3 | 2.3515 | 1.3971 | | 1.4761 | 2.6350 | 3.2573 | 2.6712 | 2.6306 | 1.0920 | 1.1003 | C4 | 2.9242 | 2.3968 | 1.4761 | | 1.1590 | 3.8902 | 2.6431 | 3.3324 | 2.0968 | 2.0942 | N5 | 3.7300 | 3.4280 | 2.6350 | 1.1590 | | 4.6537 | 3.1387 | 4.1679 | 3.1615 | 3.1505 | H6 | 1.0890 | 2.0164 | 3.2573 | 3.8902 | 4.6537 | | 1.7823 | 1.7839 | 4.0225 | 3.5898 | H7 | 1.0964 | 2.0829 | 2.6712 | 2.6431 | 3.1387 | 1.7823 | | 1.7889 | 3.6679 | 3.0246 | H8 | 1.0978 | 2.0794 | 2.6306 | 3.3324 | 4.1679 | 1.7839 | 1.7889 | | 3.5868 | 2.4144 | H9 | 3.2687 | 2.0117 | 1.0920 | 2.0968 | 3.1615 | 4.0225 | 3.6679 | 3.5868 | | 1.7763 | H10 | 2.6168 | 2.0747 | 1.1003 | 2.0942 | 3.1505 | 3.5898 | 3.0246 | 2.4144 | 1.7763 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
113.445 |
|
O2 |
C1 |
H6 |
106.509 |
| O2 |
C1 |
H7 |
111.404 |
|
O2 |
C1 |
H8 |
111.018 |
| O2 |
C3 |
C4 |
113.038 |
|
O2 |
C3 |
H9 |
107.205 |
| O2 |
C3 |
H10 |
111.803 |
|
C3 |
C4 |
N5 |
179.287 |
| C4 |
C3 |
H9 |
108.548 |
|
C4 |
C3 |
H10 |
107.864 |
| H6 |
C1 |
H7 |
109.290 |
|
H6 |
C1 |
H8 |
109.325 |
| H7 |
C1 |
H8 |
109.233 |
|
H9 |
C3 |
H10 |
108.244 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.282 |
|
|
|
| 2 |
O |
-0.300 |
|
|
|
| 3 |
C |
-0.099 |
|
|
|
| 4 |
C |
0.296 |
|
|
|
| 5 |
N |
-0.475 |
|
|
|
| 6 |
H |
0.170 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
| 8 |
H |
0.142 |
|
|
|
| 9 |
H |
0.201 |
|
|
|
| 10 |
H |
0.180 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.579 |
1.240 |
1.504 |
3.233 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.755 |
-5.796 |
0.733 |
| y |
-5.796 |
-28.166 |
0.690 |
| z |
0.733 |
0.690 |
-30.077 |
|
| Traceless |
| | x | y | z |
| x |
-7.633 |
-5.796 |
0.733 |
| y |
-5.796 |
5.250 |
0.690 |
| z |
0.733 |
0.690 |
2.383 |
|
| Polar |
| 3z2-r2 | 4.766 |
| x2-y2 | -8.589 |
| xy | -5.796 |
| xz | 0.733 |
| yz | 0.690 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.629 |
0.593 |
0.178 |
| y |
0.593 |
6.147 |
0.209 |
| z |
0.178 |
0.209 |
5.095 |
<r2> (average value of r
2) Å
2
| <r2> |
122.829 |
| (<r2>)1/2 |
11.083 |