Jump to
S1C2
Energy calculated at MP2/3-21G
| | hartrees |
| Energy at 0K | -207.139075 |
| Energy at 298.15K | -207.144955 |
| HF Energy | -206.719211 |
| Nuclear repulsion energy | 114.268718 |
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 MP2/3-21G
| 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 |
3495 |
3336 |
19.37 |
|
|
|
| 2 |
A |
3182 |
3037 |
13.35 |
|
|
|
| 3 |
A |
3166 |
3022 |
1.39 |
|
|
|
| 4 |
A |
3087 |
2947 |
10.42 |
|
|
|
| 5 |
A |
1626 |
1552 |
6.47 |
|
|
|
| 6 |
A |
1568 |
1496 |
3.11 |
|
|
|
| 7 |
A |
1488 |
1421 |
8.76 |
|
|
|
| 8 |
A |
1417 |
1352 |
10.92 |
|
|
|
| 9 |
A |
1276 |
1218 |
57.99 |
|
|
|
| 10 |
A |
1166 |
1113 |
7.69 |
|
|
|
| 11 |
A |
980 |
936 |
46.16 |
|
|
|
| 12 |
A |
881 |
841 |
12.63 |
|
|
|
| 13 |
A |
537 |
513 |
16.84 |
|
|
|
| 14 |
A |
309 |
295 |
1.62 |
|
|
|
| 15 |
A |
3151 |
3008 |
12.32 |
|
|
|
| 16 |
A |
1587 |
1515 |
9.83 |
|
|
|
| 17 |
A |
1142 |
1090 |
0.23 |
|
|
|
| 18 |
A |
935 |
892 |
23.95 |
|
|
|
| 19 |
A |
331 |
316 |
144.70 |
|
|
|
| 20 |
A |
271 |
259 |
19.87 |
|
|
|
| 21 |
A |
198 |
189 |
0.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15896.8 cm
-1
Scaled (by 0.9545) Zero Point Vibrational Energy (zpe) 15173.5 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 MP2/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.278 |
1.375 |
0.000 |
| C2 |
0.000 |
0.566 |
0.000 |
| N3 |
-0.064 |
-0.731 |
0.000 |
| O4 |
1.348 |
-1.261 |
0.000 |
| H5 |
1.161 |
-2.239 |
0.000 |
| H6 |
-2.135 |
0.695 |
0.000 |
| H7 |
-1.327 |
2.015 |
0.888 |
| H8 |
-1.327 |
2.015 |
-0.888 |
| H9 |
0.959 |
1.081 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5127 | 2.4312 | 3.7208 | 4.3597 | 1.0936 | 1.0956 | 1.0956 | 2.2568 |
C2 | 1.5127 | | 1.2988 | 2.2704 | 3.0353 | 2.1387 | 2.1561 | 2.1561 | 1.0886 | N3 | 2.4312 | 1.2988 | | 1.5077 | 1.9421 | 2.5146 | 3.1504 | 3.1504 | 2.0807 | O4 | 3.7208 | 2.2704 | 1.5077 | | 0.9950 | 3.9943 | 4.3215 | 4.3215 | 2.3737 | H5 | 4.3597 | 3.0353 | 1.9421 | 0.9950 | | 4.4122 | 5.0070 | 5.0070 | 3.3252 | H6 | 1.0936 | 2.1387 | 2.5146 | 3.9943 | 4.4122 | | 1.7841 | 1.7841 | 3.1180 | H7 | 1.0956 | 2.1561 | 3.1504 | 4.3215 | 5.0070 | 1.7841 | | 1.7758 | 2.6246 | H8 | 1.0956 | 2.1561 | 3.1504 | 4.3215 | 5.0070 | 1.7841 | 1.7758 | | 2.6246 | H9 | 2.2568 | 1.0886 | 2.0807 | 2.3737 | 3.3252 | 3.1180 | 2.6246 | 2.6246 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
119.514 |
|
C1 |
C2 |
H9 |
119.462 |
| C2 |
C1 |
H6 |
109.230 |
|
C2 |
C1 |
H7 |
110.487 |
| C2 |
C1 |
H8 |
110.487 |
|
C2 |
N3 |
O4 |
107.766 |
| N3 |
C2 |
H9 |
121.023 |
|
N3 |
O4 |
H5 |
99.763 |
| H6 |
C1 |
H7 |
109.165 |
|
H6 |
C1 |
H8 |
109.165 |
| H7 |
C1 |
H8 |
108.278 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at MP2/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.602 |
|
|
-0.428 |
| 2 |
C |
0.067 |
|
|
0.350 |
| 3 |
N |
-0.212 |
|
|
-0.313 |
| 4 |
O |
-0.454 |
|
|
-0.443 |
| 5 |
H |
0.366 |
|
|
0.418 |
| 6 |
H |
0.216 |
|
|
0.129 |
| 7 |
H |
0.205 |
|
|
0.122 |
| 8 |
H |
0.205 |
|
|
0.122 |
| 9 |
H |
0.208 |
|
|
0.043 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.505 |
0.468 |
0.000 |
0.689 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.496 |
0.432 |
0.000 |
0.658 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.948 |
-1.986 |
0.000 |
| y |
-1.986 |
-18.625 |
0.000 |
| z |
0.000 |
0.000 |
-25.218 |
|
| Traceless |
| | x | y | z |
| x |
-4.027 |
-1.986 |
0.000 |
| y |
-1.986 |
6.958 |
0.000 |
| z |
0.000 |
0.000 |
-2.931 |
|
| Polar |
| 3z2-r2 | -5.862 |
| x2-y2 | -7.323 |
| xy | -1.986 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.482 |
-1.227 |
0.000 |
| y |
-1.227 |
6.100 |
0.000 |
| z |
0.000 |
0.000 |
2.399 |
<r2> (average value of r
2) Å
2
| <r2> |
95.298 |
| (<r2>)1/2 |
9.762 |
Jump to
S1C1
Energy calculated at MP2/3-21G
| | hartrees |
| Energy at 0K | -207.139981 |
| Energy at 298.15K | |
| HF Energy | -206.719688 |
| Nuclear repulsion energy | 117.102027 |
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 MP2/3-21G
| 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' |
3503 |
3344 |
20.71 |
|
|
|
| 2 |
A' |
3222 |
3076 |
2.81 |
|
|
|
| 3 |
A' |
3189 |
3044 |
12.95 |
|
|
|
| 4 |
A' |
3093 |
2953 |
9.49 |
|
|
|
| 5 |
A' |
1629 |
1555 |
0.06 |
|
|
|
| 6 |
A' |
1571 |
1499 |
11.87 |
|
|
|
| 7 |
A' |
1479 |
1412 |
17.71 |
|
|
|
| 8 |
A' |
1400 |
1336 |
1.06 |
|
|
|
| 9 |
A' |
1318 |
1258 |
59.01 |
|
|
|
| 10 |
A' |
1166 |
1113 |
25.07 |
|
|
|
| 11 |
A' |
920 |
878 |
33.91 |
|
|
|
| 12 |
A' |
857 |
818 |
28.53 |
|
|
|
| 13 |
A' |
654 |
624 |
14.49 |
|
|
|
| 14 |
A' |
320 |
306 |
3.09 |
|
|
|
| 15 |
A" |
3149 |
3005 |
11.98 |
|
|
|
| 16 |
A" |
1602 |
1529 |
12.24 |
|
|
|
| 17 |
A" |
1139 |
1087 |
0.35 |
|
|
|
| 18 |
A" |
891 |
850 |
12.90 |
|
|
|
| 19 |
A" |
468 |
446 |
15.22 |
|
|
|
| 20 |
A" |
323 |
309 |
138.66 |
|
|
|
| 21 |
A" |
39i |
37i |
2.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15926.1 cm
-1
Scaled (by 0.9545) Zero Point Vibrational Energy (zpe) 15201.5 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 MP2/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.453 |
0.477 |
0.000 |
| C2 |
0.000 |
0.897 |
0.000 |
| N3 |
1.053 |
0.131 |
0.000 |
| O4 |
0.628 |
-1.314 |
0.000 |
| H5 |
1.524 |
-1.746 |
0.000 |
| H6 |
-1.513 |
-0.611 |
0.000 |
| H7 |
-1.960 |
0.874 |
0.887 |
| H8 |
-1.960 |
0.874 |
-0.887 |
| H9 |
0.234 |
1.959 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5124 | 2.5295 | 2.7460 | 3.7156 | 1.0895 | 1.0959 | 1.0959 | 2.2448 |
C2 | 1.5124 | | 1.3015 | 2.2981 | 3.0502 | 2.1354 | 2.1514 | 2.1514 | 1.0874 | N3 | 2.5295 | 1.3015 | | 1.5062 | 1.9350 | 2.6704 | 3.2270 | 3.2270 | 2.0026 | O4 | 2.7460 | 2.2981 | 1.5062 | | 0.9945 | 2.2535 | 3.5030 | 3.5030 | 3.2962 | H5 | 3.7156 | 3.0502 | 1.9350 | 0.9945 | | 3.2421 | 4.4482 | 4.4482 | 3.9225 | H6 | 1.0895 | 2.1354 | 2.6704 | 2.2535 | 3.2421 | | 1.7861 | 1.7861 | 3.1065 | H7 | 1.0959 | 2.1514 | 3.2270 | 3.5030 | 4.4482 | 1.7861 | | 1.7743 | 2.6029 | H8 | 1.0959 | 2.1514 | 3.2270 | 3.5030 | 4.4482 | 1.7861 | 1.7743 | | 2.6029 | H9 | 2.2448 | 1.0874 | 2.0026 | 3.2962 | 3.9225 | 3.1065 | 2.6029 | 2.6029 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
127.880 |
|
C1 |
C2 |
H9 |
118.499 |
| C2 |
C1 |
H6 |
109.233 |
|
C2 |
C1 |
H7 |
110.119 |
| C2 |
C1 |
H8 |
110.119 |
|
C2 |
N3 |
O4 |
109.657 |
| N3 |
C2 |
H9 |
113.621 |
|
N3 |
O4 |
H5 |
99.349 |
| H6 |
C1 |
H7 |
109.627 |
|
H6 |
C1 |
H8 |
109.627 |
| H7 |
C1 |
H8 |
108.098 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability