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S1C2
Vibrational Frequencies calculated at LSDA/cc-pVTZ
Geometric Data calculated at LSDA/cc-pVTZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -208.127465 |
| Energy at 298.15K | -208.133427 |
| HF Energy | -208.127465 |
| Nuclear repulsion energy | 120.939415 |
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 LSDA/cc-pVTZ
| 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' |
3734 |
3693 |
112.31 |
|
|
|
| 2 |
A' |
3094 |
3060 |
3.40 |
|
|
|
| 3 |
A' |
3076 |
3043 |
2.28 |
|
|
|
| 4 |
A' |
2971 |
2938 |
6.43 |
|
|
|
| 5 |
A' |
1710 |
1692 |
8.17 |
|
|
|
| 6 |
A' |
1402 |
1386 |
25.15 |
|
|
|
| 7 |
A' |
1336 |
1322 |
36.45 |
|
|
|
| 8 |
A' |
1314 |
1300 |
25.33 |
|
|
|
| 9 |
A' |
1278 |
1264 |
37.56 |
|
|
|
| 10 |
A' |
1120 |
1108 |
8.02 |
|
|
|
| 11 |
A' |
960 |
950 |
137.65 |
|
|
|
| 12 |
A' |
917 |
907 |
27.02 |
|
|
|
| 13 |
A' |
670 |
663 |
13.22 |
|
|
|
| 14 |
A' |
318 |
314 |
1.46 |
|
|
|
| 15 |
A" |
3029 |
2996 |
3.24 |
|
|
|
| 16 |
A" |
1404 |
1389 |
11.67 |
|
|
|
| 17 |
A" |
1007 |
996 |
0.15 |
|
|
|
| 18 |
A" |
823 |
814 |
18.34 |
|
|
|
| 19 |
A" |
521 |
515 |
48.58 |
|
|
|
| 20 |
A" |
408 |
403 |
65.92 |
|
|
|
| 21 |
A" |
38 |
37 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15564.5 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 15394.8 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 LSDA/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.420 |
0.476 |
0.000 |
| C2 |
0.000 |
0.864 |
0.000 |
| N3 |
1.004 |
0.083 |
0.000 |
| O4 |
0.638 |
-1.249 |
0.000 |
| H5 |
1.499 |
-1.700 |
0.000 |
| H6 |
-1.523 |
-0.616 |
0.000 |
| H7 |
-1.935 |
0.886 |
0.882 |
| H8 |
-1.935 |
0.886 |
-0.882 |
| H9 |
0.280 |
1.923 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4718 | 2.4555 | 2.6850 | 3.6400 | 1.0959 | 1.1009 | 1.1009 | 2.2320 |
C2 | 1.4718 | | 1.2722 | 2.2074 | 2.9697 | 2.1231 | 2.1267 | 2.1267 | 1.0950 | N3 | 2.4555 | 1.2722 | | 1.3816 | 1.8501 | 2.6218 | 3.1724 | 3.1724 | 1.9773 | O4 | 2.6850 | 2.2074 | 1.3816 | | 0.9716 | 2.2519 | 3.4583 | 3.4583 | 3.1921 | H5 | 3.6400 | 2.9697 | 1.8501 | 0.9716 | | 3.2103 | 4.3885 | 4.3885 | 3.8221 | H6 | 1.0959 | 2.1231 | 2.6218 | 2.2519 | 3.2103 | | 1.7897 | 1.7897 | 3.1131 | H7 | 1.1009 | 2.1267 | 3.1724 | 3.4583 | 4.3885 | 1.7897 | | 1.7633 | 2.5995 | H8 | 1.1009 | 2.1267 | 3.1724 | 3.4583 | 4.3885 | 1.7897 | 1.7633 | | 2.5995 | H9 | 2.2320 | 1.0950 | 1.9773 | 3.1921 | 3.8221 | 3.1131 | 2.5995 | 2.5995 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
126.830 |
|
C1 |
C2 |
H9 |
120.097 |
| C2 |
C1 |
H6 |
110.701 |
|
C2 |
C1 |
H7 |
110.691 |
| C2 |
C1 |
H8 |
110.691 |
|
C2 |
N3 |
O4 |
112.498 |
| N3 |
C2 |
H9 |
113.073 |
|
N3 |
O4 |
H5 |
102.258 |
| H6 |
C1 |
H7 |
109.111 |
|
H6 |
C1 |
H8 |
109.111 |
| H7 |
C1 |
H8 |
106.424 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.333 |
|
|
|
| 2 |
C |
-0.126 |
|
|
|
| 3 |
N |
-0.062 |
|
|
|
| 4 |
O |
-0.209 |
|
|
|
| 5 |
H |
0.216 |
|
|
|
| 6 |
H |
0.125 |
|
|
|
| 7 |
H |
0.127 |
|
|
|
| 8 |
H |
0.127 |
|
|
|
| 9 |
H |
0.135 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.666 |
-0.042 |
0.000 |
0.667 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.208 |
-4.015 |
0.000 |
| y |
-4.015 |
-21.092 |
0.000 |
| z |
0.000 |
0.000 |
-25.357 |
|
| Traceless |
| | x | y | z |
| x |
0.016 |
-4.015 |
0.000 |
| y |
-4.015 |
3.191 |
0.000 |
| z |
0.000 |
0.000 |
-3.207 |
|
| Polar |
| 3z2-r2 | -6.414 |
| x2-y2 | -2.116 |
| xy | -4.015 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.534 |
-1.187 |
0.000 |
| y |
-1.187 |
6.532 |
0.000 |
| z |
0.000 |
0.000 |
3.937 |
<r2> (average value of r
2) Å
2
| <r2> |
77.505 |
| (<r2>)1/2 |
8.804 |