Jump to
S1C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -192.939549 |
| Energy at 298.15K | -192.946798 |
| HF Energy | -192.740479 |
| Nuclear repulsion energy | 128.119075 |
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/6-311G*
| 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 |
3105 |
3105 |
31.25 |
|
|
|
| 2 |
A1 |
3061 |
3061 |
3.07 |
|
|
|
| 3 |
A1 |
1580 |
1580 |
0.03 |
|
|
|
| 4 |
A1 |
1526 |
1526 |
4.25 |
|
|
|
| 5 |
A1 |
1407 |
1407 |
2.58 |
|
|
|
| 6 |
A1 |
1059 |
1059 |
5.97 |
|
|
|
| 7 |
A1 |
936 |
936 |
31.76 |
|
|
|
| 8 |
A1 |
822 |
822 |
4.50 |
|
|
|
| 9 |
A2 |
3102 |
3102 |
0.00 |
|
|
|
| 10 |
A2 |
1261 |
1261 |
0.00 |
|
|
|
| 11 |
A2 |
1184 |
1184 |
0.00 |
|
|
|
| 12 |
A2 |
857 |
857 |
0.00 |
|
|
|
| 13 |
B1 |
3163 |
3163 |
49.18 |
|
|
|
| 14 |
B1 |
3099 |
3099 |
86.18 |
|
|
|
| 15 |
B1 |
1218 |
1218 |
0.63 |
|
|
|
| 16 |
B1 |
1170 |
1170 |
2.73 |
|
|
|
| 17 |
B1 |
779 |
779 |
0.11 |
|
|
|
| 18 |
B1 |
63 |
63 |
2.81 |
|
|
|
| 19 |
B2 |
3052 |
3052 |
168.03 |
|
|
|
| 20 |
B2 |
1551 |
1551 |
2.01 |
|
|
|
| 21 |
B2 |
1335 |
1335 |
0.62 |
|
|
|
| 22 |
B2 |
1285 |
1285 |
11.87 |
|
|
|
| 23 |
B2 |
1044 |
1044 |
96.19 |
|
|
|
| 24 |
B2 |
960 |
960 |
6.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19308.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19308.7 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/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.073 |
| C2 |
0.000 |
0.000 |
-1.076 |
| C3 |
0.000 |
1.036 |
0.063 |
| C4 |
0.000 |
-1.036 |
0.063 |
| H5 |
0.889 |
0.000 |
-1.706 |
| H6 |
-0.889 |
0.000 |
-1.706 |
| H7 |
0.892 |
1.664 |
0.133 |
| H8 |
-0.892 |
1.664 |
0.133 |
| H9 |
-0.892 |
-1.664 |
0.133 |
| H10 |
0.892 |
-1.664 |
0.133 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1489 | 1.4460 | 1.4460 | 2.9169 | 2.9169 | 2.1093 | 2.1093 | 2.1093 | 2.1093 |
C2 | 2.1489 | | 1.5398 | 1.5398 | 1.0893 | 1.0893 | 2.2421 | 2.2421 | 2.2421 | 2.2421 | C3 | 1.4460 | 1.5398 | | 2.0711 | 2.2342 | 2.2342 | 1.0935 | 1.0935 | 2.8442 | 2.8442 | C4 | 1.4460 | 1.5398 | 2.0711 | | 2.2342 | 2.2342 | 2.8442 | 2.8442 | 1.0935 | 1.0935 | H5 | 2.9169 | 1.0893 | 2.2342 | 2.2342 | | 1.7785 | 2.4796 | 3.0530 | 3.0530 | 2.4796 | H6 | 2.9169 | 1.0893 | 2.2342 | 2.2342 | 1.7785 | | 3.0530 | 2.4796 | 2.4796 | 3.0530 | H7 | 2.1093 | 2.2421 | 1.0935 | 2.8442 | 2.4796 | 3.0530 | | 1.7837 | 3.7765 | 3.3287 | H8 | 2.1093 | 2.2421 | 1.0935 | 2.8442 | 3.0530 | 2.4796 | 1.7837 | | 3.3287 | 3.7765 | H9 | 2.1093 | 2.2421 | 2.8442 | 1.0935 | 3.0530 | 2.4796 | 3.7765 | 3.3287 | | 1.7837 | H10 | 2.1093 | 2.2421 | 2.8442 | 1.0935 | 2.4796 | 3.0530 | 3.3287 | 3.7765 | 1.7837 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.005 |
|
O1 |
C3 |
H7 |
111.567 |
| O1 |
C3 |
H8 |
111.567 |
|
O1 |
C4 |
C2 |
92.005 |
| O1 |
C4 |
H9 |
111.567 |
|
O1 |
C4 |
H10 |
111.567 |
| C2 |
C3 |
H7 |
115.699 |
|
C2 |
C3 |
H8 |
115.699 |
| C2 |
C4 |
H9 |
115.699 |
|
C2 |
C4 |
H10 |
115.699 |
| C3 |
O1 |
C4 |
91.471 |
|
C3 |
C2 |
C4 |
84.519 |
| C3 |
C2 |
H5 |
115.306 |
|
C3 |
C2 |
H6 |
115.306 |
| C4 |
C2 |
H5 |
115.306 |
|
C4 |
C2 |
H6 |
115.306 |
| H5 |
C2 |
H6 |
109.443 |
|
H7 |
C3 |
H8 |
109.301 |
| H9 |
C4 |
H10 |
109.301 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.357 |
|
|
|
| 2 |
C |
-0.554 |
|
|
|
| 3 |
C |
-0.155 |
|
|
|
| 4 |
C |
-0.155 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
| 6 |
H |
0.223 |
|
|
|
| 7 |
H |
0.194 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
| 9 |
H |
0.194 |
|
|
|
| 10 |
H |
0.194 |
|
|
|
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 |
-2.018 |
2.018 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.301 |
0.000 |
0.000 |
| y |
0.000 |
-23.164 |
0.000 |
| z |
0.000 |
0.000 |
-28.135 |
|
| Traceless |
| | x | y | z |
| x |
1.348 |
0.000 |
0.000 |
| y |
0.000 |
3.054 |
0.000 |
| z |
0.000 |
0.000 |
-4.402 |
|
| Polar |
| 3z2-r2 | -8.804 |
| x2-y2 | -1.137 |
| 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 |
4.768 |
0.000 |
0.000 |
| y |
0.000 |
5.804 |
0.000 |
| z |
0.000 |
0.000 |
4.757 |
<r2> (average value of r
2) Å
2
| <r2> |
66.541 |
| (<r2>)1/2 |
8.157 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -192.939549 |
| Energy at 298.15K | -192.946798 |
| HF Energy | -192.740481 |
| Nuclear repulsion energy | 128.121963 |
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/6-311G*
| 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' |
3162 |
3162 |
49.36 |
|
|
|
| 2 |
A' |
3105 |
3105 |
31.26 |
|
|
|
| 3 |
A' |
3099 |
3099 |
86.04 |
|
|
|
| 4 |
A' |
3061 |
3061 |
3.08 |
|
|
|
| 5 |
A' |
1580 |
1580 |
0.04 |
|
|
|
| 6 |
A' |
1526 |
1526 |
4.25 |
|
|
|
| 7 |
A' |
1407 |
1407 |
2.58 |
|
|
|
| 8 |
A' |
1218 |
1218 |
0.63 |
|
|
|
| 9 |
A' |
1170 |
1170 |
2.74 |
|
|
|
| 10 |
A' |
1059 |
1059 |
5.97 |
|
|
|
| 11 |
A' |
936 |
936 |
31.77 |
|
|
|
| 12 |
A' |
822 |
822 |
4.50 |
|
|
|
| 13 |
A' |
779 |
779 |
0.11 |
|
|
|
| 14 |
A' |
63 |
63 |
2.81 |
|
|
|
| 15 |
A" |
3102 |
3102 |
0.00 |
|
|
|
| 16 |
A" |
3052 |
3052 |
168.06 |
|
|
|
| 17 |
A" |
1552 |
1552 |
2.01 |
|
|
|
| 18 |
A" |
1335 |
1335 |
0.62 |
|
|
|
| 19 |
A" |
1285 |
1285 |
11.86 |
|
|
|
| 20 |
A" |
1261 |
1261 |
0.00 |
|
|
|
| 21 |
A" |
1184 |
1184 |
0.00 |
|
|
|
| 22 |
A" |
1044 |
1044 |
96.21 |
|
|
|
| 23 |
A" |
960 |
960 |
6.28 |
|
|
|
| 24 |
A" |
857 |
857 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19308.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19308.9 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
-1.073 |
0.000 |
| C2 |
-0.000 |
1.076 |
0.000 |
| C3 |
0.000 |
-0.063 |
1.036 |
| C4 |
0.000 |
-0.063 |
-1.036 |
| H5 |
0.889 |
1.706 |
0.000 |
| H6 |
-0.889 |
1.706 |
0.000 |
| H7 |
0.892 |
-0.133 |
1.664 |
| H8 |
-0.892 |
-0.132 |
1.664 |
| H9 |
0.892 |
-0.133 |
-1.664 |
| H10 |
-0.892 |
-0.132 |
-1.664 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1488 | 1.4460 | 1.4460 | 2.9170 | 2.9169 | 2.1092 | 2.1093 | 2.1092 | 2.1093 |
C2 | 2.1488 | | 1.5398 | 1.5398 | 1.0893 | 1.0893 | 2.2421 | 2.2420 | 2.2421 | 2.2420 | C3 | 1.4460 | 1.5398 | | 2.0710 | 2.2342 | 2.2342 | 1.0935 | 1.0935 | 2.8442 | 2.8442 | C4 | 1.4460 | 1.5398 | 2.0710 | | 2.2342 | 2.2342 | 2.8442 | 2.8442 | 1.0935 | 1.0935 | H5 | 2.9170 | 1.0893 | 2.2342 | 2.2342 | | 1.7783 | 2.4798 | 3.0529 | 2.4798 | 3.0529 | H6 | 2.9169 | 1.0893 | 2.2342 | 2.2342 | 1.7783 | | 3.0530 | 2.4795 | 3.0530 | 2.4795 | H7 | 2.1092 | 2.2421 | 1.0935 | 2.8442 | 2.4798 | 3.0530 | | 1.7837 | 3.3287 | 3.7765 | H8 | 2.1093 | 2.2420 | 1.0935 | 2.8442 | 3.0529 | 2.4795 | 1.7837 | | 3.7765 | 3.3286 | H9 | 2.1092 | 2.2421 | 2.8442 | 1.0935 | 2.4798 | 3.0530 | 3.3287 | 3.7765 | | 1.7837 | H10 | 2.1093 | 2.2420 | 2.8442 | 1.0935 | 3.0529 | 2.4795 | 3.7765 | 3.3286 | 1.7837 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.003 |
|
O1 |
C3 |
H7 |
111.566 |
| O1 |
C3 |
H8 |
111.573 |
|
O1 |
C4 |
C2 |
92.003 |
| O1 |
C4 |
H9 |
111.566 |
|
O1 |
C4 |
H10 |
111.573 |
| C2 |
C3 |
H7 |
115.704 |
|
C2 |
C3 |
H8 |
115.692 |
| C2 |
C4 |
H9 |
115.704 |
|
C2 |
C4 |
H10 |
115.692 |
| C3 |
O1 |
C4 |
91.472 |
|
C3 |
C2 |
C4 |
84.522 |
| C3 |
C2 |
H5 |
115.315 |
|
C3 |
C2 |
H6 |
115.310 |
| C4 |
C2 |
H5 |
115.315 |
|
C4 |
C2 |
H6 |
115.310 |
| H5 |
C2 |
H6 |
109.422 |
|
H7 |
C3 |
H8 |
109.300 |
| H9 |
C4 |
H10 |
109.300 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.357 |
|
|
|
| 2 |
C |
-0.554 |
|
|
|
| 3 |
C |
-0.155 |
|
|
|
| 4 |
C |
-0.155 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
| 6 |
H |
0.223 |
|
|
|
| 7 |
H |
0.194 |
|
|
|
| 8 |
H |
0.194 |
|
|
|
| 9 |
H |
0.194 |
|
|
|
| 10 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
2.018 |
0.000 |
2.018 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.302 |
-0.000 |
0.000 |
| y |
-0.000 |
-28.134 |
0.000 |
| z |
0.000 |
0.000 |
-23.164 |
|
| Traceless |
| | x | y | z |
| x |
1.347 |
-0.000 |
0.000 |
| y |
-0.000 |
-4.401 |
0.000 |
| z |
0.000 |
0.000 |
3.054 |
|
| Polar |
| 3z2-r2 | 6.108 |
| x2-y2 | 3.832 |
| 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 |
4.768 |
-0.000 |
0.000 |
| y |
-0.000 |
4.757 |
0.000 |
| z |
0.000 |
0.000 |
5.803 |
<r2> (average value of r
2) Å
2
| <r2> |
66.539 |
| (<r2>)1/2 |
8.157 |