Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -191.947983 |
| Energy at 298.15K | -191.955212 |
| HF Energy | -191.947983 |
| Nuclear repulsion energy | 126.171477 |
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 B1B95/3-21G
| 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 |
3138 |
3002 |
16.30 |
|
|
|
| 2 |
A1 |
3102 |
2968 |
5.19 |
|
|
|
| 3 |
A1 |
1597 |
1527 |
0.22 |
|
|
|
| 4 |
A1 |
1529 |
1463 |
4.82 |
|
|
|
| 5 |
A1 |
1373 |
1314 |
0.64 |
|
|
|
| 6 |
A1 |
1026 |
982 |
0.15 |
|
|
|
| 7 |
A1 |
887 |
849 |
12.15 |
|
|
|
| 8 |
A1 |
804 |
769 |
5.38 |
|
|
|
| 9 |
A2 |
3150 |
3013 |
0.00 |
|
|
|
| 10 |
A2 |
1275 |
1220 |
0.00 |
|
|
|
| 11 |
A2 |
1141 |
1091 |
0.00 |
|
|
|
| 12 |
A2 |
877 |
839 |
0.00 |
|
|
|
| 13 |
B1 |
3202 |
3063 |
29.77 |
|
|
|
| 14 |
B1 |
3149 |
3013 |
55.88 |
|
|
|
| 15 |
B1 |
1214 |
1162 |
2.11 |
|
|
|
| 16 |
B1 |
1102 |
1054 |
0.33 |
|
|
|
| 17 |
B1 |
765 |
732 |
1.65 |
|
|
|
| 18 |
B1 |
75 |
72 |
3.20 |
|
|
|
| 19 |
B2 |
3092 |
2958 |
106.69 |
|
|
|
| 20 |
B2 |
1566 |
1498 |
0.86 |
|
|
|
| 21 |
B2 |
1315 |
1258 |
20.70 |
|
|
|
| 22 |
B2 |
1286 |
1230 |
3.15 |
|
|
|
| 23 |
B2 |
1007 |
963 |
52.51 |
|
|
|
| 24 |
B2 |
940 |
900 |
15.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19305.2 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 18469.2 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 B1B95/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.103 |
| C2 |
0.000 |
0.000 |
-1.077 |
| C3 |
0.000 |
1.063 |
0.052 |
| C4 |
0.000 |
-1.063 |
0.052 |
| H5 |
0.894 |
0.000 |
-1.699 |
| H6 |
-0.894 |
0.000 |
-1.699 |
| H7 |
0.896 |
1.682 |
0.102 |
| H8 |
-0.896 |
1.682 |
0.102 |
| H9 |
-0.896 |
-1.682 |
0.102 |
| H10 |
0.896 |
-1.682 |
0.102 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1809 | 1.4947 | 1.4947 | 2.9415 | 2.9415 | 2.1528 | 2.1528 | 2.1528 | 2.1528 |
C2 | 2.1809 | | 1.5509 | 1.5509 | 1.0885 | 1.0885 | 2.2413 | 2.2413 | 2.2413 | 2.2413 | C3 | 1.4947 | 1.5509 | | 2.1252 | 2.2348 | 2.2348 | 1.0904 | 1.0904 | 2.8876 | 2.8876 | C4 | 1.4947 | 1.5509 | 2.1252 | | 2.2348 | 2.2348 | 2.8876 | 2.8876 | 1.0904 | 1.0904 | H5 | 2.9415 | 1.0885 | 2.2348 | 2.2348 | | 1.7871 | 2.4644 | 3.0456 | 3.0456 | 2.4644 | H6 | 2.9415 | 1.0885 | 2.2348 | 2.2348 | 1.7871 | | 3.0456 | 2.4644 | 2.4644 | 3.0456 | H7 | 2.1528 | 2.2413 | 1.0904 | 2.8876 | 2.4644 | 3.0456 | | 1.7920 | 3.8115 | 3.3640 | H8 | 2.1528 | 2.2413 | 1.0904 | 2.8876 | 3.0456 | 2.4644 | 1.7920 | | 3.3640 | 3.8115 | H9 | 2.1528 | 2.2413 | 2.8876 | 1.0904 | 3.0456 | 2.4644 | 3.8115 | 3.3640 | | 1.7920 | H10 | 2.1528 | 2.2413 | 2.8876 | 1.0904 | 2.4644 | 3.0456 | 3.3640 | 3.8115 | 1.7920 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.443 |
|
O1 |
C3 |
H7 |
111.817 |
| O1 |
C3 |
H8 |
111.817 |
|
O1 |
C4 |
C2 |
91.443 |
| O1 |
C4 |
H9 |
111.817 |
|
O1 |
C4 |
H10 |
111.817 |
| C2 |
C3 |
H7 |
114.995 |
|
C2 |
C3 |
H8 |
114.995 |
| C2 |
C4 |
H9 |
114.995 |
|
C2 |
C4 |
H10 |
114.995 |
| C3 |
O1 |
C4 |
90.618 |
|
C3 |
C2 |
C4 |
86.496 |
| C3 |
C2 |
H5 |
114.580 |
|
C3 |
C2 |
H6 |
114.580 |
| C4 |
C2 |
H5 |
114.580 |
|
C4 |
C2 |
H6 |
114.580 |
| H5 |
C2 |
H6 |
110.350 |
|
H7 |
C3 |
H8 |
110.515 |
| H9 |
C4 |
H10 |
110.515 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.473 |
|
|
|
| 2 |
C |
-0.530 |
|
|
|
| 3 |
C |
-0.155 |
|
|
|
| 4 |
C |
-0.155 |
|
|
|
| 5 |
H |
0.230 |
|
|
|
| 6 |
H |
0.230 |
|
|
|
| 7 |
H |
0.214 |
|
|
|
| 8 |
H |
0.214 |
|
|
|
| 9 |
H |
0.214 |
|
|
|
| 10 |
H |
0.214 |
|
|
|
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 |
-2.320 |
2.320 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.971 |
0.000 |
0.000 |
| y |
0.000 |
-22.286 |
0.000 |
| z |
0.000 |
0.000 |
-27.931 |
|
| Traceless |
| | x | y | z |
| x |
1.138 |
0.000 |
0.000 |
| y |
0.000 |
3.665 |
0.000 |
| z |
0.000 |
0.000 |
-4.803 |
|
| Polar |
| 3z2-r2 | -9.605 |
| x2-y2 | -1.685 |
| 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 |
4.273 |
0.000 |
0.000 |
| y |
0.000 |
5.406 |
0.000 |
| z |
0.000 |
0.000 |
4.104 |
<r2> (average value of r
2) Å
2
| <r2> |
67.673 |
| (<r2>)1/2 |
8.226 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -191.947983 |
| Energy at 298.15K | -191.955213 |
| HF Energy | -191.947983 |
| Nuclear repulsion energy | 126.170115 |
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 B1B95/3-21G
| 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' |
3202 |
3063 |
29.89 |
|
|
|
| 2 |
A' |
3149 |
3012 |
55.78 |
|
|
|
| 3 |
A' |
3138 |
3002 |
16.30 |
|
|
|
| 4 |
A' |
3102 |
2968 |
5.20 |
|
|
|
| 5 |
A' |
1597 |
1527 |
0.23 |
|
|
|
| 6 |
A' |
1529 |
1463 |
4.82 |
|
|
|
| 7 |
A' |
1373 |
1314 |
0.64 |
|
|
|
| 8 |
A' |
1214 |
1162 |
2.11 |
|
|
|
| 9 |
A' |
1102 |
1054 |
0.32 |
|
|
|
| 10 |
A' |
1026 |
982 |
0.15 |
|
|
|
| 11 |
A' |
887 |
849 |
12.15 |
|
|
|
| 12 |
A' |
804 |
769 |
5.38 |
|
|
|
| 13 |
A' |
765 |
732 |
1.65 |
|
|
|
| 14 |
A' |
76 |
73 |
3.20 |
|
|
|
| 15 |
A" |
3149 |
3013 |
0.00 |
|
|
|
| 16 |
A" |
3092 |
2958 |
106.71 |
|
|
|
| 17 |
A" |
1566 |
1498 |
0.86 |
|
|
|
| 18 |
A" |
1315 |
1258 |
20.74 |
|
|
|
| 19 |
A" |
1286 |
1230 |
3.11 |
|
|
|
| 20 |
A" |
1275 |
1220 |
0.00 |
|
|
|
| 21 |
A" |
1141 |
1091 |
0.00 |
|
|
|
| 22 |
A" |
1007 |
963 |
52.38 |
|
|
|
| 23 |
A" |
941 |
900 |
15.49 |
|
|
|
| 24 |
A" |
877 |
839 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19305.1 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 18469.2 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 B1B95/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.001 |
-1.104 |
0.000 |
| C2 |
-0.000 |
1.077 |
0.000 |
| C3 |
-0.000 |
-0.052 |
1.063 |
| C4 |
-0.000 |
-0.052 |
-1.063 |
| H5 |
0.893 |
1.699 |
0.000 |
| H6 |
-0.894 |
1.699 |
0.000 |
| H7 |
0.895 |
-0.102 |
1.683 |
| H8 |
-0.897 |
-0.103 |
1.681 |
| H9 |
0.895 |
-0.102 |
-1.683 |
| H10 |
-0.897 |
-0.103 |
-1.681 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1809 | 1.4948 | 1.4948 | 2.9412 | 2.9423 | 2.1529 | 2.1529 | 2.1529 | 2.1529 |
C2 | 2.1809 | | 1.5508 | 1.5508 | 1.0885 | 1.0885 | 2.2413 | 2.2411 | 2.2413 | 2.2411 | C3 | 1.4948 | 1.5508 | | 2.1251 | 2.2348 | 2.2350 | 1.0904 | 1.0904 | 2.8881 | 2.8870 | C4 | 1.4948 | 1.5508 | 2.1251 | | 2.2348 | 2.2350 | 2.8881 | 2.8870 | 1.0904 | 1.0904 | H5 | 2.9412 | 1.0885 | 2.2348 | 2.2348 | | 1.7869 | 2.4646 | 3.0458 | 2.4646 | 3.0458 | H6 | 2.9423 | 1.0885 | 2.2350 | 2.2350 | 1.7869 | | 3.0455 | 2.4645 | 3.0455 | 2.4645 | H7 | 2.1529 | 2.2413 | 1.0904 | 2.8881 | 2.4646 | 3.0455 | | 1.7919 | 3.3656 | 3.8116 | H8 | 2.1529 | 2.2411 | 1.0904 | 2.8870 | 3.0458 | 2.4645 | 1.7919 | | 3.8116 | 3.3626 | H9 | 2.1529 | 2.2413 | 2.8881 | 1.0904 | 2.4646 | 3.0455 | 3.3656 | 3.8116 | | 1.7919 | H10 | 2.1529 | 2.2411 | 2.8870 | 1.0904 | 3.0458 | 2.4645 | 3.8116 | 3.3626 | 1.7919 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.448 |
|
O1 |
C3 |
H7 |
111.819 |
| O1 |
C3 |
H8 |
111.818 |
|
O1 |
C4 |
C2 |
91.448 |
| O1 |
C4 |
H9 |
111.819 |
|
O1 |
C4 |
H10 |
111.818 |
| C2 |
C3 |
H7 |
115.007 |
|
C2 |
C3 |
H8 |
114.989 |
| C2 |
C4 |
H9 |
115.007 |
|
C2 |
C4 |
H10 |
114.989 |
| C3 |
O1 |
C4 |
90.606 |
|
C3 |
C2 |
C4 |
86.497 |
| C3 |
C2 |
H5 |
114.581 |
|
C3 |
C2 |
H6 |
114.597 |
| C4 |
C2 |
H5 |
114.581 |
|
C4 |
C2 |
H6 |
114.597 |
| H5 |
C2 |
H6 |
110.322 |
|
H7 |
C3 |
H8 |
110.505 |
| H9 |
C4 |
H10 |
110.505 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.473 |
|
|
|
| 2 |
C |
-0.530 |
|
|
|
| 3 |
C |
-0.155 |
|
|
|
| 4 |
C |
-0.155 |
|
|
|
| 5 |
H |
0.230 |
|
|
|
| 6 |
H |
0.230 |
|
|
|
| 7 |
H |
0.214 |
|
|
|
| 8 |
H |
0.214 |
|
|
|
| 9 |
H |
0.214 |
|
|
|
| 10 |
H |
0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.003 |
2.321 |
0.000 |
2.321 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.972 |
0.004 |
0.000 |
| y |
0.004 |
-27.930 |
0.000 |
| z |
0.000 |
0.000 |
-22.285 |
|
| Traceless |
| | x | y | z |
| x |
1.135 |
0.004 |
0.000 |
| y |
0.004 |
-4.801 |
0.000 |
| z |
0.000 |
0.000 |
3.666 |
|
| Polar |
| 3z2-r2 | 7.331 |
| x2-y2 | 3.958 |
| xy | 0.004 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.273 |
0.000 |
0.000 |
| y |
0.000 |
4.105 |
0.000 |
| z |
0.000 |
0.000 |
5.406 |
<r2> (average value of r
2) Å
2
| <r2> |
67.675 |
| (<r2>)1/2 |
8.226 |