Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -209.106534 |
| Energy at 298.15K | -209.112464 |
| Nuclear repulsion energy | 115.019326 |
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 |
3691 |
3548 |
45.31 |
|
|
|
| 2 |
A |
3167 |
3044 |
24.23 |
|
|
|
| 3 |
A |
3136 |
3015 |
8.01 |
|
|
|
| 4 |
A |
3040 |
2922 |
21.23 |
|
|
|
| 5 |
A |
1684 |
1619 |
1.58 |
|
|
|
| 6 |
A |
1505 |
1446 |
16.31 |
|
|
|
| 7 |
A |
1444 |
1388 |
7.03 |
|
|
|
| 8 |
A |
1400 |
1346 |
30.49 |
|
|
|
| 9 |
A |
1258 |
1209 |
51.14 |
|
|
|
| 10 |
A |
1159 |
1114 |
10.20 |
|
|
|
| 11 |
A |
990 |
952 |
89.26 |
|
|
|
| 12 |
A |
869 |
836 |
47.74 |
|
|
|
| 13 |
A |
543 |
522 |
19.40 |
|
|
|
| 14 |
A |
311 |
299 |
3.08 |
|
|
|
| 15 |
A |
3113 |
2992 |
26.39 |
|
|
|
| 16 |
A |
1507 |
1448 |
18.82 |
|
|
|
| 17 |
A |
1096 |
1053 |
0.56 |
|
|
|
| 18 |
A |
926 |
890 |
26.09 |
|
|
|
| 19 |
A |
403 |
387 |
198.31 |
|
|
|
| 20 |
A |
279 |
268 |
1.14 |
|
|
|
| 21 |
A |
195 |
187 |
0.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15857.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15242.2 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/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.284 |
1.357 |
0.000 |
| C2 |
0.000 |
0.573 |
0.000 |
| N3 |
-0.034 |
-0.724 |
0.000 |
| O4 |
1.328 |
-1.261 |
0.000 |
| H5 |
1.189 |
-2.233 |
0.000 |
| H6 |
-2.149 |
0.687 |
0.000 |
| H7 |
-1.339 |
2.006 |
0.885 |
| H8 |
-1.339 |
2.006 |
-0.885 |
| H9 |
0.954 |
1.109 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5046 | 2.4281 | 3.6983 | 4.3593 | 1.0943 | 1.0988 | 1.0988 | 2.2513 |
C2 | 1.5046 | | 1.2976 | 2.2642 | 3.0471 | 2.1517 | 2.1516 | 2.1516 | 1.0942 | N3 | 2.4281 | 1.2976 | | 1.4637 | 1.9419 | 2.5423 | 3.1530 | 3.1530 | 2.0826 | O4 | 3.6983 | 2.2642 | 1.4637 | | 0.9813 | 3.9850 | 4.3091 | 4.3091 | 2.3997 | H5 | 4.3593 | 3.0471 | 1.9419 | 0.9813 | | 4.4344 | 5.0141 | 5.0141 | 3.3502 | H6 | 1.0943 | 2.1517 | 2.5423 | 3.9850 | 4.4344 | | 1.7835 | 1.7835 | 3.1310 | H7 | 1.0988 | 2.1516 | 3.1530 | 4.3091 | 5.0141 | 1.7835 | | 1.7698 | 2.6157 | H8 | 1.0988 | 2.1516 | 3.1530 | 4.3091 | 5.0141 | 1.7835 | 1.7698 | | 2.6157 | H9 | 2.2513 | 1.0942 | 2.0826 | 2.3997 | 3.3502 | 3.1310 | 2.6157 | 2.6157 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
119.930 |
|
C1 |
C2 |
H9 |
119.218 |
| C2 |
C1 |
H6 |
110.783 |
|
C2 |
C1 |
H7 |
110.510 |
| C2 |
C1 |
H8 |
110.510 |
|
C2 |
N3 |
O4 |
110.021 |
| N3 |
C2 |
H9 |
120.852 |
|
N3 |
O4 |
H5 |
103.395 |
| H6 |
C1 |
H7 |
108.828 |
|
H6 |
C1 |
H8 |
108.828 |
| H7 |
C1 |
H8 |
107.290 |
|
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 |
-0.645 |
|
|
|
| 2 |
C |
-0.111 |
|
|
|
| 3 |
N |
-0.037 |
|
|
|
| 4 |
O |
-0.466 |
|
|
|
| 5 |
H |
0.369 |
|
|
|
| 6 |
H |
0.231 |
|
|
|
| 7 |
H |
0.215 |
|
|
|
| 8 |
H |
0.215 |
|
|
|
| 9 |
H |
0.228 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.583 |
0.902 |
0.000 |
1.074 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.681 |
-2.271 |
0.000 |
| y |
-2.271 |
-17.899 |
0.000 |
| z |
0.000 |
0.000 |
-25.121 |
|
| Traceless |
| | x | y | z |
| x |
-4.171 |
-2.271 |
0.000 |
| y |
-2.271 |
7.502 |
0.000 |
| z |
0.000 |
0.000 |
-3.331 |
|
| Polar |
| 3z2-r2 | -6.663 |
| x2-y2 | -7.782 |
| xy | -2.271 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.965 |
-1.487 |
0.000 |
| y |
-1.487 |
6.901 |
0.000 |
| z |
0.000 |
0.000 |
2.827 |
<r2> (average value of r
2) Å
2
| <r2> |
94.551 |
| (<r2>)1/2 |
9.724 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -209.107588 |
| Energy at 298.15K | -209.113542 |
| HF Energy | -209.107588 |
| Nuclear repulsion energy | 117.554290 |
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' |
3696 |
3552 |
44.54 |
|
|
|
| 2 |
A' |
3198 |
3074 |
14.70 |
|
|
|
| 3 |
A' |
3180 |
3056 |
3.76 |
|
|
|
| 4 |
A' |
3047 |
2928 |
14.87 |
|
|
|
| 5 |
A' |
1698 |
1632 |
5.55 |
|
|
|
| 6 |
A' |
1501 |
1443 |
21.79 |
|
|
|
| 7 |
A' |
1434 |
1378 |
29.25 |
|
|
|
| 8 |
A' |
1361 |
1308 |
0.63 |
|
|
|
| 9 |
A' |
1310 |
1259 |
79.84 |
|
|
|
| 10 |
A' |
1150 |
1106 |
15.04 |
|
|
|
| 11 |
A' |
933 |
897 |
43.41 |
|
|
|
| 12 |
A' |
856 |
823 |
90.88 |
|
|
|
| 13 |
A' |
660 |
635 |
14.11 |
|
|
|
| 14 |
A' |
299 |
287 |
2.44 |
|
|
|
| 15 |
A" |
3116 |
2995 |
23.29 |
|
|
|
| 16 |
A" |
1517 |
1458 |
21.14 |
|
|
|
| 17 |
A" |
1084 |
1042 |
0.35 |
|
|
|
| 18 |
A" |
875 |
841 |
21.95 |
|
|
|
| 19 |
A" |
495 |
476 |
45.49 |
|
|
|
| 20 |
A" |
397 |
381 |
138.75 |
|
|
|
| 21 |
A" |
67 |
64 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15935.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15317.1 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 Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.460 |
0.510 |
0.000 |
| C2 |
0.000 |
0.882 |
0.000 |
| N3 |
1.037 |
0.099 |
0.000 |
| O4 |
0.652 |
-1.312 |
0.000 |
| H5 |
1.517 |
-1.774 |
0.000 |
| H6 |
-1.592 |
-0.574 |
0.000 |
| H7 |
-1.955 |
0.933 |
0.884 |
| H8 |
-1.955 |
0.933 |
-0.884 |
| H9 |
0.272 |
1.938 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5065 | 2.5303 | 2.7890 | 3.7522 | 1.0915 | 1.0987 | 1.0987 | 2.2448 |
C2 | 1.5065 | | 1.2992 | 2.2884 | 3.0584 | 2.1572 | 2.1466 | 2.1466 | 1.0907 | N3 | 2.5303 | 1.2992 | | 1.4623 | 1.9332 | 2.7139 | 3.2298 | 3.2298 | 1.9917 | O4 | 2.7890 | 2.2884 | 1.4623 | | 0.9810 | 2.3627 | 3.5526 | 3.5526 | 3.2719 | H5 | 3.7522 | 3.0584 | 1.9332 | 0.9810 | | 3.3334 | 4.4911 | 4.4911 | 3.9149 | H6 | 1.0915 | 2.1572 | 2.7139 | 2.3627 | 3.3334 | | 1.7847 | 1.7847 | 3.1280 | H7 | 1.0987 | 2.1466 | 3.2298 | 3.5526 | 4.4911 | 1.7847 | | 1.7689 | 2.5986 | H8 | 1.0987 | 2.1466 | 3.2298 | 3.5526 | 4.4911 | 1.7847 | 1.7689 | | 2.5986 | H9 | 2.2448 | 1.0907 | 1.9917 | 3.2719 | 3.9149 | 3.1280 | 2.5986 | 2.5986 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.655 |
|
C1 |
C2 |
H9 |
118.741 |
| C2 |
C1 |
H6 |
111.264 |
|
C2 |
C1 |
H7 |
109.987 |
| C2 |
C1 |
H8 |
109.987 |
|
C2 |
N3 |
O4 |
111.795 |
| N3 |
C2 |
H9 |
112.604 |
|
N3 |
O4 |
H5 |
102.818 |
| H6 |
C1 |
H7 |
109.141 |
|
H6 |
C1 |
H8 |
109.141 |
| H7 |
C1 |
H8 |
107.227 |
|
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 |
-0.662 |
|
|
|
| 2 |
C |
-0.149 |
|
|
|
| 3 |
N |
-0.012 |
|
|
|
| 4 |
O |
-0.478 |
|
|
|
| 5 |
H |
0.375 |
|
|
|
| 6 |
H |
0.265 |
|
|
|
| 7 |
H |
0.217 |
|
|
|
| 8 |
H |
0.217 |
|
|
|
| 9 |
H |
0.226 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.797 |
0.480 |
0.000 |
0.931 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.912 |
-4.379 |
0.000 |
| y |
-4.379 |
-20.779 |
0.000 |
| z |
0.000 |
0.000 |
-25.213 |
|
| Traceless |
| | x | y | z |
| x |
0.085 |
-4.379 |
0.000 |
| y |
-4.379 |
3.283 |
0.000 |
| z |
0.000 |
0.000 |
-3.368 |
|
| Polar |
| 3z2-r2 | -6.735 |
| x2-y2 | -2.132 |
| xy | -4.379 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.540 |
-1.375 |
0.000 |
| y |
-1.375 |
6.019 |
0.000 |
| z |
0.000 |
0.000 |
2.886 |
<r2> (average value of r
2) Å
2
| <r2> |
81.216 |
| (<r2>)1/2 |
9.012 |