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S2C1
Vibrational Frequencies calculated at B2PLYP=FULLultrafine/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 |
Ag |
3175 |
3033 |
0.00 |
212.33 |
0.12 |
0.21 |
| 2 |
Ag |
1693 |
1617 |
0.00 |
11.45 |
0.01 |
0.02 |
| 3 |
Ag |
1388 |
1326 |
0.00 |
33.08 |
0.34 |
0.51 |
| 4 |
Au |
1074 |
1026 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
B1u |
3158 |
3018 |
14.97 |
0.00 |
0.00 |
0.00 |
| 6 |
B1u |
1490 |
1424 |
9.20 |
0.00 |
0.00 |
0.00 |
| 7 |
B2g |
981 |
937 |
0.00 |
2.11 |
0.75 |
0.86 |
| 8 |
B2u |
3258 |
3113 |
20.81 |
0.00 |
0.33 |
0.50 |
| 9 |
B2u |
837 |
800 |
0.15 |
0.00 |
0.33 |
0.50 |
| 10 |
B3g |
3229 |
3085 |
0.00 |
119.95 |
0.75 |
0.86 |
| 11 |
B3g |
1253 |
1197 |
0.00 |
0.40 |
0.75 |
0.86 |
| 12 |
B3u |
987 |
943 |
93.54 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 11262.3 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 10760.0 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/cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.663 |
| C2 |
0.000 |
0.000 |
-0.663 |
| H3 |
0.000 |
0.920 |
1.228 |
| H4 |
0.000 |
-0.920 |
1.228 |
| H5 |
0.000 |
-0.920 |
-1.228 |
| H6 |
0.000 |
0.920 |
-1.228 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
| C1 | | 1.3263 | 1.0796 | 1.0796 | 2.1032 | 2.1032 |
C2 | 1.3263 | | 2.1032 | 2.1032 | 1.0796 | 1.0796 | H3 | 1.0796 | 2.1032 | | 1.8397 | 3.0690 | 2.4565 | H4 | 1.0796 | 2.1032 | 1.8397 | | 2.4565 | 3.0690 | H5 | 2.1032 | 1.0796 | 3.0690 | 2.4565 | | 1.8397 | H6 | 2.1032 | 1.0796 | 2.4565 | 3.0690 | 1.8397 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H5 |
121.566 |
|
C1 |
C2 |
H6 |
121.566 |
| C2 |
C1 |
H3 |
121.566 |
|
C2 |
C1 |
H4 |
121.566 |
| H3 |
C1 |
H4 |
116.869 |
|
H5 |
C2 |
H6 |
116.869 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.262 |
|
|
|
| 2 |
C |
-0.262 |
|
|
|
| 3 |
H |
0.131 |
|
|
|
| 4 |
H |
0.131 |
|
|
|
| 5 |
H |
0.131 |
|
|
|
| 6 |
H |
0.131 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.559 |
0.000 |
0.000 |
| y |
0.000 |
-12.415 |
0.000 |
| z |
0.000 |
0.000 |
-12.350 |
|
| Traceless |
| | x | y | z |
| x |
-3.176 |
0.000 |
0.000 |
| y |
0.000 |
1.539 |
0.000 |
| z |
0.000 |
0.000 |
1.637 |
|
| Polar |
| 3z2-r2 | 3.274 |
| x2-y2 | -3.144 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.284 |
0.000 |
0.000 |
| y |
0.000 |
3.342 |
0.000 |
| z |
0.000 |
0.000 |
4.971 |
<r2> (average value of r
2) Å
2
| <r2> |
23.091 |
| (<r2>)1/2 |
4.805 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/cc-pVTZ
| | hartrees |
| Energy at 0K | -78.441799 |
| Energy at 298.15K | |
| HF Energy | -78.337361 |
| Nuclear repulsion energy | 31.977941 |
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/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 |
A1 |
3129 |
2989 |
0.00 |
263.14 |
0.03 |
0.06 |
| 2 |
A1 |
1469 |
1404 |
0.00 |
21.95 |
0.55 |
0.71 |
| 3 |
A1 |
1145 |
1094 |
0.00 |
0.98 |
0.10 |
0.18 |
| 4 |
B1 |
716 |
684 |
0.00 |
6.05 |
0.75 |
0.86 |
| 5 |
B2 |
3135 |
2995 |
19.78 |
53.87 |
0.75 |
0.86 |
| 6 |
B2 |
1448 |
1384 |
0.45 |
0.01 |
0.75 |
0.86 |
| 7 |
E |
3211 |
3068 |
7.23 |
72.98 |
0.75 |
0.86 |
| 7 |
E |
3211 |
3068 |
7.23 |
72.98 |
0.75 |
0.86 |
| 8 |
E |
942 |
900 |
1.05 |
0.93 |
0.75 |
0.86 |
| 8 |
E |
942 |
900 |
1.05 |
0.93 |
0.75 |
0.86 |
| 9 |
E |
425 |
406 |
53.36 |
0.58 |
0.75 |
0.86 |
| 9 |
E |
425 |
406 |
53.36 |
0.58 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 10098.8 cm
-1
Scaled (by 0.9554) Zero Point Vibrational Energy (zpe) 9648.4 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/cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.722 |
| C2 |
0.000 |
0.000 |
-0.722 |
| H3 |
0.000 |
0.921 |
1.290 |
| H4 |
0.000 |
-0.921 |
1.290 |
| H5 |
0.921 |
0.000 |
-1.290 |
| H6 |
-0.921 |
0.000 |
-1.290 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
| C1 | | 1.4447 | 1.0814 | 1.0814 | 2.2126 | 2.2126 |
C2 | 1.4447 | | 2.2126 | 2.2126 | 1.0814 | 1.0814 | H3 | 1.0814 | 2.2126 | | 1.8412 | 2.8893 | 2.8893 | H4 | 1.0814 | 2.2126 | 1.8412 | | 2.8893 | 2.8893 | H5 | 2.2126 | 1.0814 | 2.8893 | 2.8893 | | 1.8412 | H6 | 2.2126 | 1.0814 | 2.8893 | 2.8893 | 1.8412 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.268 |
|
|
|
| 2 |
C |
-0.268 |
|
|
|
| 3 |
H |
0.134 |
|
|
|
| 4 |
H |
0.134 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
| 6 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.058 |
0.000 |
0.000 |
| y |
0.000 |
-14.051 |
0.000 |
| z |
0.000 |
0.000 |
-13.166 |
|
| Traceless |
| | x | y | z |
| x |
-0.449 |
0.000 |
0.000 |
| y |
0.000 |
-0.439 |
0.000 |
| z |
0.000 |
0.000 |
0.889 |
|
| Polar |
| 3z2-r2 | 1.778 |
| x2-y2 | -0.007 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.934 |
0.000 |
0.000 |
| y |
0.000 |
2.932 |
0.000 |
| z |
0.000 |
0.000 |
4.368 |
<r2> (average value of r
2) Å
2
| <r2> |
24.898 |
| (<r2>)1/2 |
4.990 |