Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pCVTZ
| | hartrees |
| Energy at 0K | -191.895420 |
| Energy at 298.15K | |
| HF Energy | -191.601259 |
| Nuclear repulsion energy | 103.258124 |
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 B2PLYP=FULLultrafine/aug-cc-pCVTZ
| 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' |
3254 |
3254 |
3.55 |
64.55 |
0.51 |
0.68 |
| 2 |
A' |
3201 |
3201 |
0.92 |
97.26 |
0.27 |
0.43 |
| 3 |
A' |
3158 |
3158 |
4.27 |
87.27 |
0.08 |
0.14 |
| 4 |
A' |
2918 |
2918 |
82.99 |
111.25 |
0.26 |
0.41 |
| 5 |
A' |
1748 |
1748 |
237.40 |
93.58 |
0.35 |
0.51 |
| 6 |
A' |
1672 |
1672 |
3.22 |
31.77 |
0.09 |
0.16 |
| 7 |
A' |
1464 |
1464 |
10.39 |
6.40 |
0.44 |
0.61 |
| 8 |
A' |
1393 |
1393 |
5.33 |
22.29 |
0.27 |
0.42 |
| 9 |
A' |
1306 |
1306 |
2.72 |
11.48 |
0.14 |
0.25 |
| 10 |
A' |
1180 |
1180 |
39.23 |
13.06 |
0.61 |
0.75 |
| 11 |
A' |
928 |
928 |
19.74 |
1.54 |
0.01 |
0.01 |
| 12 |
A' |
573 |
573 |
4.06 |
6.32 |
0.16 |
0.28 |
| 13 |
A' |
322 |
322 |
10.37 |
1.04 |
0.31 |
0.47 |
| 14 |
A" |
1038 |
1038 |
12.98 |
0.25 |
0.75 |
0.86 |
| 15 |
A" |
1027 |
1027 |
5.01 |
1.82 |
0.75 |
0.86 |
| 16 |
A" |
1001 |
1001 |
37.85 |
2.61 |
0.75 |
0.86 |
| 17 |
A" |
616 |
616 |
10.40 |
0.66 |
0.75 |
0.86 |
| 18 |
A" |
165 |
165 |
4.57 |
0.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13481.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 13481.1 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 B2PLYP=FULLultrafine/aug-cc-pCVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.149 |
-0.741 |
0.000 |
| C2 |
0.000 |
0.720 |
0.000 |
| C3 |
1.210 |
1.280 |
0.000 |
| O4 |
-1.214 |
-1.320 |
0.000 |
| H5 |
0.803 |
-1.305 |
0.000 |
| H6 |
-0.910 |
1.304 |
0.000 |
| H7 |
1.348 |
2.350 |
0.000 |
| H8 |
2.102 |
0.666 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4688 | 2.4353 | 1.2126 | 1.1064 | 2.1827 | 3.4348 | 2.6542 |
C2 | 1.4688 | | 1.3333 | 2.3741 | 2.1783 | 1.0813 | 2.1155 | 2.1024 | C3 | 2.4353 | 1.3333 | | 3.5548 | 2.6162 | 2.1201 | 1.0793 | 1.0822 | O4 | 1.2126 | 2.3741 | 3.5548 | | 2.0177 | 2.6422 | 4.4763 | 3.8652 | H5 | 1.1064 | 2.1783 | 2.6162 | 2.0177 | | 3.1213 | 3.6952 | 2.3600 | H6 | 2.1827 | 1.0813 | 2.1201 | 2.6422 | 3.1213 | | 2.4884 | 3.0783 | H7 | 3.4348 | 2.1155 | 1.0793 | 4.4763 | 3.6952 | 2.4884 | | 1.8448 | H8 | 2.6542 | 2.1024 | 1.0822 | 3.8652 | 2.3600 | 3.0783 | 1.8448 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.627 |
|
C1 |
C2 |
H6 |
116.908 |
| C2 |
C1 |
O4 |
124.326 |
|
C2 |
C1 |
H5 |
114.808 |
| C2 |
C3 |
H7 |
122.172 |
|
C2 |
C3 |
H8 |
120.644 |
| C3 |
C2 |
H6 |
122.465 |
|
O4 |
C1 |
H5 |
120.866 |
| H7 |
C3 |
H8 |
117.185 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.017 |
|
|
|
| 2 |
C |
-0.338 |
|
|
|
| 3 |
C |
-0.932 |
|
|
|
| 4 |
O |
-0.616 |
|
|
|
| 5 |
H |
0.475 |
|
|
|
| 6 |
H |
0.546 |
|
|
|
| 7 |
H |
0.457 |
|
|
|
| 8 |
H |
0.391 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.572 |
2.165 |
0.000 |
3.362 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.989 |
-2.750 |
-0.006 |
| y |
-2.750 |
-24.357 |
-0.007 |
| z |
-0.006 |
-0.007 |
-25.205 |
|
| Traceless |
| | x | y | z |
| x |
-0.208 |
-2.750 |
-0.006 |
| y |
-2.750 |
0.740 |
-0.007 |
| z |
-0.006 |
-0.007 |
-0.532 |
|
| Polar |
| 3z2-r2 | -1.065 |
| x2-y2 | -0.632 |
| xy | -2.750 |
| xz | -0.006 |
| yz | -0.007 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.705 |
1.726 |
0.001 |
| y |
1.726 |
7.274 |
0.001 |
| z |
0.001 |
0.001 |
4.223 |
<r2> (average value of r
2) Å
2
| <r2> |
83.489 |
| (<r2>)1/2 |
9.137 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pCVTZ
| | hartrees |
| Energy at 0K | -191.891758 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
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 B2PLYP=FULLultrafine/aug-cc-pCVTZ
Geometric Data calculated at B2PLYP=FULLultrafine/aug-cc-pCVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability