Jump to
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -247.231348 |
| Energy at 298.15K | -247.236954 |
| HF Energy | -247.231348 |
| Nuclear repulsion energy | 157.744861 |
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 wB97X-D/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' |
3172 |
3172 |
21.38 |
|
|
|
| 2 |
A' |
3004 |
3004 |
57.47 |
|
|
|
| 3 |
A' |
2997 |
2997 |
29.20 |
|
|
|
| 4 |
A' |
2414 |
2414 |
0.51 |
|
|
|
| 5 |
A' |
1538 |
1538 |
7.07 |
|
|
|
| 6 |
A' |
1516 |
1516 |
8.87 |
|
|
|
| 7 |
A' |
1503 |
1503 |
1.65 |
|
|
|
| 8 |
A' |
1443 |
1443 |
38.39 |
|
|
|
| 9 |
A' |
1256 |
1256 |
61.57 |
|
|
|
| 10 |
A' |
1195 |
1195 |
131.68 |
|
|
|
| 11 |
A' |
1027 |
1027 |
39.47 |
|
|
|
| 12 |
A' |
966 |
966 |
7.07 |
|
|
|
| 13 |
A' |
559 |
559 |
1.68 |
|
|
|
| 14 |
A' |
393 |
393 |
1.95 |
|
|
|
| 15 |
A' |
186 |
186 |
2.44 |
|
|
|
| 16 |
A" |
3056 |
3056 |
54.65 |
|
|
|
| 17 |
A" |
3031 |
3031 |
42.17 |
|
|
|
| 18 |
A" |
1511 |
1511 |
11.54 |
|
|
|
| 19 |
A" |
1294 |
1294 |
4.21 |
|
|
|
| 20 |
A" |
1200 |
1200 |
3.41 |
|
|
|
| 21 |
A" |
1041 |
1041 |
2.23 |
|
|
|
| 22 |
A" |
381 |
381 |
1.71 |
|
|
|
| 23 |
A" |
221 |
221 |
4.72 |
|
|
|
| 24 |
A" |
87 |
87 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17495.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17495.2 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 wB97X-D/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-2.120 |
-0.361 |
0.000 |
| O2 |
-0.734 |
-0.604 |
0.000 |
| C3 |
0.000 |
0.584 |
0.000 |
| C4 |
1.431 |
0.271 |
0.000 |
| N5 |
2.560 |
0.058 |
0.000 |
| H6 |
-2.609 |
-1.334 |
0.000 |
| H7 |
-2.430 |
0.198 |
0.893 |
| H8 |
-2.430 |
0.198 |
-0.893 |
| H9 |
-0.219 |
1.197 |
-0.887 |
| H10 |
-0.219 |
1.197 |
0.887 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4074 | 2.3217 | 3.6073 | 4.6987 | 1.0883 | 1.0986 | 1.0986 | 2.6135 | 2.6135 |
O2 | 1.4074 | | 1.3963 | 2.3350 | 3.3594 | 2.0125 | 2.0779 | 2.0779 | 2.0723 | 2.0723 | C3 | 2.3217 | 1.3963 | | 1.4649 | 2.6130 | 3.2384 | 2.6180 | 2.6180 | 1.1004 | 1.1004 | C4 | 3.6073 | 2.3350 | 1.4649 | | 1.1484 | 4.3475 | 3.9640 | 3.9640 | 2.0900 | 2.0900 | N5 | 4.6987 | 3.3594 | 2.6130 | 1.1484 | | 5.3531 | 5.0711 | 5.0711 | 3.1314 | 3.1314 | H6 | 1.0883 | 2.0125 | 3.2384 | 4.3475 | 5.3531 | | 1.7820 | 1.7820 | 3.5924 | 3.5924 | H7 | 1.0986 | 2.0779 | 2.6180 | 3.9640 | 5.0711 | 1.7820 | | 1.7869 | 3.0097 | 2.4264 | H8 | 1.0986 | 2.0779 | 2.6180 | 3.9640 | 5.0711 | 1.7820 | 1.7869 | | 2.4264 | 3.0097 | H9 | 2.6135 | 2.0723 | 1.1004 | 2.0900 | 3.1314 | 3.5924 | 3.0097 | 2.4264 | | 1.7744 | H10 | 2.6135 | 2.0723 | 1.1004 | 2.0900 | 3.1314 | 3.5924 | 2.4264 | 3.0097 | 1.7744 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
111.806 |
|
O2 |
C1 |
H6 |
106.793 |
| O2 |
C1 |
H7 |
111.436 |
|
O2 |
C1 |
H8 |
111.436 |
| O2 |
C3 |
C4 |
109.371 |
|
O2 |
C3 |
H9 |
111.658 |
| O2 |
C3 |
H10 |
111.658 |
|
C3 |
C4 |
N5 |
178.332 |
| C4 |
C3 |
H9 |
108.283 |
|
C4 |
C3 |
H10 |
108.283 |
| H6 |
C1 |
H7 |
109.143 |
|
H6 |
C1 |
H8 |
109.143 |
| H7 |
C1 |
H8 |
108.831 |
|
H9 |
C3 |
H10 |
107.466 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.459 |
|
|
|
| 2 |
O |
-0.317 |
|
|
|
| 3 |
C |
-0.218 |
|
|
|
| 4 |
C |
0.099 |
|
|
|
| 5 |
N |
-0.237 |
|
|
|
| 6 |
H |
0.242 |
|
|
|
| 7 |
H |
0.206 |
|
|
|
| 8 |
H |
0.206 |
|
|
|
| 9 |
H |
0.239 |
|
|
|
| 10 |
H |
0.239 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-4.425 |
1.803 |
0.000 |
4.778 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.084 |
0.726 |
0.000 |
| y |
0.726 |
-29.164 |
0.000 |
| z |
0.000 |
0.000 |
-29.111 |
|
| Traceless |
| | x | y | z |
| x |
-6.947 |
0.726 |
0.000 |
| y |
0.726 |
3.433 |
0.000 |
| z |
0.000 |
0.000 |
3.513 |
|
| Polar |
| 3z2-r2 | 7.027 |
| x2-y2 | -6.920 |
| xy | 0.726 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.001 |
-0.016 |
0.000 |
| y |
-0.016 |
4.830 |
0.000 |
| z |
0.000 |
0.000 |
4.557 |
<r2> (average value of r
2) Å
2
| <r2> |
141.898 |
| (<r2>)1/2 |
11.912 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -247.234236 |
| Energy at 298.15K | -247.239974 |
| HF Energy | -247.234236 |
| Nuclear repulsion energy | 160.554479 |
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 wB97X-D/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 |
3171 |
3171 |
22.51 |
|
|
|
| 2 |
A |
3139 |
3139 |
6.43 |
|
|
|
| 3 |
A |
3079 |
3079 |
44.14 |
|
|
|
| 4 |
A |
3021 |
3021 |
40.35 |
|
|
|
| 5 |
A |
3014 |
3014 |
40.10 |
|
|
|
| 6 |
A |
2396 |
2396 |
0.15 |
|
|
|
| 7 |
A |
1534 |
1534 |
11.88 |
|
|
|
| 8 |
A |
1516 |
1516 |
13.69 |
|
|
|
| 9 |
A |
1512 |
1512 |
0.53 |
|
|
|
| 10 |
A |
1498 |
1498 |
3.45 |
|
|
|
| 11 |
A |
1419 |
1419 |
16.48 |
|
|
|
| 12 |
A |
1344 |
1344 |
8.96 |
|
|
|
| 13 |
A |
1249 |
1249 |
59.89 |
|
|
|
| 14 |
A |
1205 |
1205 |
12.39 |
|
|
|
| 15 |
A |
1191 |
1191 |
91.85 |
|
|
|
| 16 |
A |
1052 |
1052 |
7.68 |
|
|
|
| 17 |
A |
973 |
973 |
35.81 |
|
|
|
| 18 |
A |
908 |
908 |
22.60 |
|
|
|
| 19 |
A |
611 |
611 |
1.61 |
|
|
|
| 20 |
A |
408 |
408 |
2.84 |
|
|
|
| 21 |
A |
372 |
372 |
1.26 |
|
|
|
| 22 |
A |
264 |
264 |
11.23 |
|
|
|
| 23 |
A |
183 |
183 |
3.80 |
|
|
|
| 24 |
A |
122 |
122 |
8.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17589.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 17589.0 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 wB97X-D/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.561 |
-0.767 |
0.133 |
| O2 |
1.076 |
0.433 |
-0.429 |
| C3 |
-0.062 |
0.926 |
0.205 |
| C4 |
-1.244 |
0.054 |
0.034 |
| N5 |
-2.151 |
-0.639 |
-0.094 |
| H6 |
2.473 |
-1.017 |
-0.405 |
| H7 |
0.838 |
-1.584 |
0.021 |
| H8 |
1.792 |
-0.638 |
1.199 |
| H9 |
-0.281 |
1.898 |
-0.238 |
| H10 |
0.099 |
1.068 |
1.283 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
C3 |
C4 |
N5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.4121 | 2.3465 | 2.9241 | 3.7214 | 1.0883 | 1.0965 | 1.0981 | 3.2613 | 2.6133 |
O2 | 1.4121 | | 1.3928 | 2.3957 | 3.4173 | 2.0141 | 2.0811 | 2.0768 | 2.0059 | 2.0715 | C3 | 2.3465 | 1.3928 | | 1.4783 | 2.6275 | 3.2518 | 2.6731 | 2.6214 | 1.0908 | 1.0996 | C4 | 2.9241 | 2.3957 | 1.4783 | | 1.1493 | 3.8929 | 2.6494 | 3.3245 | 2.0981 | 2.0956 | N5 | 3.7214 | 3.4173 | 2.6275 | 1.1493 | | 4.6501 | 3.1375 | 4.1502 | 3.1556 | 3.1427 | H6 | 1.0883 | 2.0141 | 3.2518 | 3.8929 | 4.6501 | | 1.7820 | 1.7836 | 4.0140 | 3.5828 | H7 | 1.0965 | 2.0811 | 2.6731 | 2.6494 | 3.1375 | 1.7820 | | 1.7871 | 3.6673 | 3.0293 | H8 | 1.0981 | 2.0768 | 2.6214 | 3.3245 | 4.1502 | 1.7836 | 1.7871 | | 3.5771 | 2.4053 | H9 | 3.2613 | 2.0059 | 1.0908 | 2.0981 | 3.1556 | 4.0140 | 3.6673 | 3.5771 | | 1.7741 | H10 | 2.6133 | 2.0715 | 1.0996 | 2.0956 | 3.1427 | 3.5828 | 3.0293 | 2.4053 | 1.7741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
C3 |
113.559 |
|
O2 |
C1 |
H6 |
106.604 |
| O2 |
C1 |
H7 |
111.491 |
|
O2 |
C1 |
H8 |
111.035 |
| O2 |
C3 |
C4 |
113.081 |
|
O2 |
C3 |
H9 |
107.114 |
| O2 |
C3 |
H10 |
111.896 |
|
C3 |
C4 |
N5 |
179.024 |
| C4 |
C3 |
H9 |
108.567 |
|
C4 |
C3 |
H10 |
107.852 |
| H6 |
C1 |
H7 |
109.300 |
|
H6 |
C1 |
H8 |
109.319 |
| H7 |
C1 |
H8 |
109.038 |
|
H9 |
C3 |
H10 |
108.185 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.468 |
|
|
|
| 2 |
O |
-0.310 |
|
|
|
| 3 |
C |
-0.261 |
|
|
|
| 4 |
C |
0.095 |
|
|
|
| 5 |
N |
-0.241 |
|
|
|
| 6 |
H |
0.236 |
|
|
|
| 7 |
H |
0.231 |
|
|
|
| 8 |
H |
0.203 |
|
|
|
| 9 |
H |
0.268 |
|
|
|
| 10 |
H |
0.246 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.554 |
1.248 |
1.425 |
3.180 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.219 |
-5.656 |
0.636 |
| y |
-5.656 |
-27.906 |
0.604 |
| z |
0.636 |
0.604 |
-29.667 |
|
| Traceless |
| | x | y | z |
| x |
-7.433 |
-5.656 |
0.636 |
| y |
-5.656 |
5.037 |
0.604 |
| z |
0.636 |
0.604 |
2.396 |
|
| Polar |
| 3z2-r2 | 4.791 |
| x2-y2 | -8.313 |
| xy | -5.656 |
| xz | 0.636 |
| yz | 0.604 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.837 |
0.460 |
0.169 |
| y |
0.460 |
5.604 |
0.227 |
| z |
0.169 |
0.227 |
4.557 |
<r2> (average value of r
2) Å
2
| <r2> |
122.189 |
| (<r2>)1/2 |
11.054 |