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S1C2
Vibrational Frequencies calculated at LSDA/6-31G*
Geometric Data calculated at LSDA/6-31G*
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at LSDA/6-31G*
| hartrees |
Energy at 0K | -229.934943 |
Energy at 298.15K | -229.940934 |
HF Energy | -229.934943 |
Nuclear repulsion energy | 162.094150 |
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/6-31G*
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 |
3227 |
3166 |
1.12 |
|
|
|
2 |
A |
3223 |
3163 |
2.18 |
|
|
|
3 |
A |
3147 |
3089 |
6.63 |
|
|
|
4 |
A |
3131 |
3072 |
0.37 |
|
|
|
5 |
A |
3129 |
3071 |
6.69 |
|
|
|
6 |
A |
3083 |
3026 |
10.72 |
|
|
|
7 |
A |
1717 |
1685 |
104.17 |
|
|
|
8 |
A |
1694 |
1662 |
172.82 |
|
|
|
9 |
A |
1391 |
1365 |
2.37 |
|
|
|
10 |
A |
1379 |
1353 |
50.44 |
|
|
|
11 |
A |
1336 |
1311 |
87.35 |
|
|
|
12 |
A |
1284 |
1260 |
9.16 |
|
|
|
13 |
A |
1255 |
1232 |
158.30 |
|
|
|
14 |
A |
1136 |
1114 |
17.56 |
|
|
|
15 |
A |
994 |
976 |
13.57 |
|
|
|
16 |
A |
968 |
950 |
10.72 |
|
|
|
17 |
A |
944 |
926 |
29.54 |
|
|
|
18 |
A |
876 |
860 |
9.91 |
|
|
|
19 |
A |
820 |
804 |
51.55 |
|
|
|
20 |
A |
802 |
787 |
60.74 |
|
|
|
21 |
A |
718 |
704 |
5.18 |
|
|
|
22 |
A |
705 |
692 |
3.21 |
|
|
|
23 |
A |
581 |
570 |
2.21 |
|
|
|
24 |
A |
447 |
439 |
2.09 |
|
|
|
25 |
A |
297 |
292 |
2.03 |
|
|
|
26 |
A |
228 |
224 |
8.20 |
|
|
|
27 |
A |
101 |
99 |
0.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19305.5 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 18944.5 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 LSDA/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-0.045 |
-0.791 |
0.041 |
C2 |
1.277 |
-0.500 |
0.009 |
C3 |
-0.908 |
0.228 |
0.283 |
C4 |
1.820 |
0.708 |
-0.146 |
C5 |
-2.154 |
0.212 |
-0.179 |
H6 |
1.869 |
-1.415 |
0.121 |
H7 |
-0.498 |
1.021 |
0.927 |
H8 |
2.907 |
0.812 |
-0.135 |
H9 |
1.220 |
1.606 |
-0.318 |
H10 |
-2.849 |
1.005 |
0.102 |
H11 |
-2.507 |
-0.594 |
-0.829 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
O1 | | 1.3539 | 1.3573 | 2.4005 | 2.3462 | 2.0141 | 2.0674 | 3.3635 | 2.7344 | 3.3313 | 2.6190 |
C2 | 1.3539 | | 2.3190 | 1.3337 | 3.5091 | 1.0955 | 2.5113 | 2.0970 | 2.1321 | 4.3932 | 3.8767 | C3 | 1.3573 | 2.3190 | | 2.8030 | 1.3294 | 3.2302 | 1.1008 | 3.8817 | 2.6053 | 2.0993 | 2.1142 | C4 | 2.4005 | 1.3337 | 2.8030 | | 4.0054 | 2.1405 | 2.5737 | 1.0917 | 1.0938 | 4.6856 | 4.5703 | C5 | 2.3462 | 3.5091 | 1.3294 | 4.0054 | | 4.3497 | 2.1498 | 5.0967 | 3.6534 | 1.0918 | 1.0936 | H6 | 2.0141 | 1.0955 | 3.2302 | 2.1405 | 4.3497 | | 3.4906 | 2.4698 | 3.1211 | 5.3027 | 4.5524 | H7 | 2.0674 | 2.5113 | 1.1008 | 2.5737 | 2.1498 | 3.4906 | | 3.5730 | 2.2011 | 2.4921 | 3.1190 | H8 | 3.3635 | 2.0970 | 3.8817 | 1.0917 | 5.0967 | 2.4698 | 3.5730 | | 1.8740 | 5.7645 | 5.6364 | H9 | 2.7344 | 2.1321 | 2.6053 | 1.0938 | 3.6534 | 3.1211 | 2.2011 | 1.8740 | | 4.1347 | 4.3580 | H10 | 3.3313 | 4.3932 | 2.0993 | 4.6856 | 1.0918 | 5.3027 | 2.4921 | 5.7645 | 4.1347 | | 1.8819 | H11 | 2.6190 | 3.8767 | 2.1142 | 4.5703 | 1.0936 | 4.5524 | 3.1190 | 5.6364 | 4.3580 | 1.8819 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C4 |
126.552 |
|
O1 |
C2 |
H6 |
110.185 |
O1 |
C3 |
C5 |
121.676 |
|
O1 |
C3 |
H7 |
114.108 |
C2 |
O1 |
C3 |
117.599 |
|
C2 |
C4 |
H8 |
119.335 |
C2 |
C4 |
H9 |
122.569 |
|
C3 |
C5 |
H10 |
119.908 |
C3 |
C5 |
H11 |
121.199 |
|
C4 |
C2 |
H6 |
123.260 |
C5 |
C3 |
H7 |
124.142 |
|
H8 |
C4 |
H9 |
118.065 |
H10 |
C5 |
H11 |
118.886 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.349 |
|
|
|
2 |
C |
0.088 |
|
|
|
3 |
C |
0.096 |
|
|
|
4 |
C |
-0.435 |
|
|
|
5 |
C |
-0.430 |
|
|
|
6 |
H |
0.172 |
|
|
|
7 |
H |
0.166 |
|
|
|
8 |
H |
0.173 |
|
|
|
9 |
H |
0.172 |
|
|
|
10 |
H |
0.172 |
|
|
|
11 |
H |
0.176 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.351 |
0.573 |
0.245 |
0.715 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.699 |
-1.575 |
0.581 |
y |
-1.575 |
-28.884 |
0.890 |
z |
0.581 |
0.890 |
-32.108 |
|
Traceless |
| x | y | z |
x |
3.797 |
-1.575 |
0.581 |
y |
-1.575 |
0.520 |
0.890 |
z |
0.581 |
0.890 |
-4.317 |
|
Polar |
3z2-r2 | -8.634 |
x2-y2 | 2.185 |
xy | -1.575 |
xz | 0.581 |
yz | 0.890 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.823 |
0.262 |
0.569 |
y |
0.262 |
6.349 |
0.303 |
z |
0.569 |
0.303 |
3.544 |
<r2> (average value of r
2) Å
2
<r2> |
129.058 |
(<r2>)1/2 |
11.360 |