Jump to
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -192.951038 |
| Energy at 298.15K | -192.958263 |
| HF Energy | -192.951038 |
| Nuclear repulsion energy | 126.863337 |
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 B1B95/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3134 |
2989 |
20.06 |
|
|
|
| 2 |
A1 |
3107 |
2963 |
6.31 |
|
|
|
| 3 |
A1 |
1583 |
1510 |
0.09 |
|
|
|
| 4 |
A1 |
1536 |
1465 |
4.40 |
|
|
|
| 5 |
A1 |
1385 |
1321 |
0.00 |
|
|
|
| 6 |
A1 |
1050 |
1001 |
0.18 |
|
|
|
| 7 |
A1 |
902 |
860 |
19.73 |
|
|
|
| 8 |
A1 |
801 |
764 |
6.20 |
|
|
|
| 9 |
A2 |
3160 |
3013 |
0.00 |
|
|
|
| 10 |
A2 |
1266 |
1207 |
0.00 |
|
|
|
| 11 |
A2 |
1146 |
1093 |
0.00 |
|
|
|
| 12 |
A2 |
875 |
834 |
0.00 |
|
|
|
| 13 |
B1 |
3199 |
3050 |
50.20 |
|
|
|
| 14 |
B1 |
3157 |
3011 |
49.98 |
|
|
|
| 15 |
B1 |
1223 |
1166 |
1.95 |
|
|
|
| 16 |
B1 |
1132 |
1079 |
0.84 |
|
|
|
| 17 |
B1 |
791 |
754 |
1.23 |
|
|
|
| 18 |
B1 |
62 |
59 |
5.07 |
|
|
|
| 19 |
B2 |
3098 |
2955 |
114.05 |
|
|
|
| 20 |
B2 |
1558 |
1486 |
0.19 |
|
|
|
| 21 |
B2 |
1331 |
1270 |
11.17 |
|
|
|
| 22 |
B2 |
1306 |
1246 |
5.90 |
|
|
|
| 23 |
B2 |
1015 |
968 |
38.44 |
|
|
|
| 24 |
B2 |
963 |
918 |
38.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19389.0 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 18491.3 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 B1B95/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.093 |
| C2 |
0.000 |
0.000 |
-1.070 |
| C3 |
0.000 |
1.056 |
0.051 |
| C4 |
0.000 |
-1.056 |
0.051 |
| H5 |
0.887 |
0.000 |
-1.703 |
| H6 |
-0.887 |
0.000 |
-1.703 |
| H7 |
0.892 |
1.680 |
0.118 |
| H8 |
-0.892 |
1.680 |
0.118 |
| H9 |
-0.892 |
-1.680 |
0.118 |
| H10 |
0.892 |
-1.680 |
0.118 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1623 | 1.4829 | 1.4829 | 2.9324 | 2.9324 | 2.1372 | 2.1372 | 2.1372 | 2.1372 |
C2 | 2.1623 | | 1.5397 | 1.5397 | 1.0893 | 1.0893 | 2.2425 | 2.2425 | 2.2425 | 2.2425 | C3 | 1.4829 | 1.5397 | | 2.1112 | 2.2306 | 2.2306 | 1.0907 | 1.0907 | 2.8781 | 2.8781 | C4 | 1.4829 | 1.5397 | 2.1112 | | 2.2306 | 2.2306 | 2.8781 | 2.8781 | 1.0907 | 1.0907 | H5 | 2.9324 | 1.0893 | 2.2306 | 2.2306 | | 1.7731 | 2.4774 | 3.0495 | 3.0495 | 2.4774 | H6 | 2.9324 | 1.0893 | 2.2306 | 2.2306 | 1.7731 | | 3.0495 | 2.4774 | 2.4774 | 3.0495 | H7 | 2.1372 | 2.2425 | 1.0907 | 2.8781 | 2.4774 | 3.0495 | | 1.7833 | 3.8041 | 3.3603 | H8 | 2.1372 | 2.2425 | 1.0907 | 2.8781 | 3.0495 | 2.4774 | 1.7833 | | 3.3603 | 3.8041 | H9 | 2.1372 | 2.2425 | 2.8781 | 1.0907 | 3.0495 | 2.4774 | 3.8041 | 3.3603 | | 1.7833 | H10 | 2.1372 | 2.2425 | 2.8781 | 1.0907 | 2.4774 | 3.0495 | 3.3603 | 3.8041 | 1.7833 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.332 |
|
O1 |
C3 |
H7 |
111.380 |
| O1 |
C3 |
H8 |
111.380 |
|
O1 |
C4 |
C2 |
91.332 |
| O1 |
C4 |
H9 |
111.380 |
|
O1 |
C4 |
H10 |
111.380 |
| C2 |
C3 |
H7 |
115.927 |
|
C2 |
C3 |
H8 |
115.927 |
| C2 |
C4 |
H9 |
115.927 |
|
C2 |
C4 |
H10 |
115.927 |
| C3 |
O1 |
C4 |
90.772 |
|
C3 |
C2 |
C4 |
86.563 |
| C3 |
C2 |
H5 |
115.021 |
|
C3 |
C2 |
H6 |
115.021 |
| C4 |
C2 |
H5 |
115.021 |
|
C4 |
C2 |
H6 |
115.021 |
| H5 |
C2 |
H6 |
108.960 |
|
H7 |
C3 |
H8 |
109.675 |
| H9 |
C4 |
H10 |
109.675 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.537 |
|
|
|
| 2 |
C |
-0.404 |
|
|
|
| 3 |
C |
-0.036 |
|
|
|
| 4 |
C |
-0.036 |
|
|
|
| 5 |
H |
0.176 |
|
|
|
| 6 |
H |
0.176 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
| 9 |
H |
0.165 |
|
|
|
| 10 |
H |
0.165 |
|
|
|
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 |
-2.541 |
2.541 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.011 |
0.000 |
0.000 |
| y |
0.000 |
-22.152 |
0.000 |
| z |
0.000 |
0.000 |
-28.340 |
|
| Traceless |
| | x | y | z |
| x |
1.235 |
0.000 |
0.000 |
| y |
0.000 |
4.023 |
0.000 |
| z |
0.000 |
0.000 |
-5.258 |
|
| Polar |
| 3z2-r2 | -10.516 |
| x2-y2 | -1.859 |
| 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 |
4.447 |
0.000 |
0.000 |
| y |
0.000 |
5.550 |
0.000 |
| z |
0.000 |
0.000 |
4.350 |
<r2> (average value of r
2) Å
2
| <r2> |
67.226 |
| (<r2>)1/2 |
8.199 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -192.951038 |
| Energy at 298.15K | -192.958264 |
| HF Energy | -192.951038 |
| Nuclear repulsion energy | 126.860677 |
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 B1B95/6-31G
| 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' |
3198 |
3050 |
50.60 |
|
|
|
| 2 |
A' |
3157 |
3011 |
49.57 |
|
|
|
| 3 |
A' |
3134 |
2989 |
20.04 |
|
|
|
| 4 |
A' |
3107 |
2963 |
6.36 |
|
|
|
| 5 |
A' |
1583 |
1510 |
0.09 |
|
|
|
| 6 |
A' |
1537 |
1466 |
4.40 |
|
|
|
| 7 |
A' |
1385 |
1321 |
0.00 |
|
|
|
| 8 |
A' |
1223 |
1166 |
1.96 |
|
|
|
| 9 |
A' |
1132 |
1079 |
0.84 |
|
|
|
| 10 |
A' |
1050 |
1001 |
0.17 |
|
|
|
| 11 |
A' |
901 |
860 |
19.72 |
|
|
|
| 12 |
A' |
801 |
764 |
6.19 |
|
|
|
| 13 |
A' |
791 |
754 |
1.26 |
|
|
|
| 14 |
A' |
63 |
60 |
5.07 |
|
|
|
| 15 |
A" |
3159 |
3013 |
0.00 |
|
|
|
| 16 |
A" |
3098 |
2955 |
114.00 |
|
|
|
| 17 |
A" |
1558 |
1486 |
0.19 |
|
|
|
| 18 |
A" |
1331 |
1270 |
11.22 |
|
|
|
| 19 |
A" |
1306 |
1246 |
5.83 |
|
|
|
| 20 |
A" |
1266 |
1207 |
0.00 |
|
|
|
| 21 |
A" |
1146 |
1093 |
0.00 |
|
|
|
| 22 |
A" |
1015 |
968 |
37.95 |
|
|
|
| 23 |
A" |
962 |
918 |
39.22 |
|
|
|
| 24 |
A" |
875 |
834 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19388.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 18491.2 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 B1B95/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.002 |
-1.093 |
0.000 |
| C2 |
-0.001 |
1.070 |
0.000 |
| C3 |
-0.001 |
-0.051 |
1.056 |
| C4 |
-0.001 |
-0.051 |
-1.056 |
| H5 |
0.886 |
1.703 |
0.000 |
| H6 |
-0.887 |
1.703 |
0.000 |
| H7 |
0.890 |
-0.117 |
1.682 |
| H8 |
-0.893 |
-0.119 |
1.679 |
| H9 |
0.890 |
-0.117 |
-1.682 |
| H10 |
-0.893 |
-0.119 |
-1.679 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1624 | 1.4830 | 1.4830 | 2.9316 | 2.9337 | 2.1373 | 2.1373 | 2.1373 | 2.1373 |
C2 | 2.1624 | | 1.5396 | 1.5396 | 1.0893 | 1.0893 | 2.2426 | 2.2422 | 2.2426 | 2.2422 | C3 | 1.4830 | 1.5396 | | 2.1112 | 2.2306 | 2.2307 | 1.0907 | 1.0907 | 2.8793 | 2.8770 | C4 | 1.4830 | 1.5396 | 2.1112 | | 2.2306 | 2.2307 | 2.8793 | 2.8770 | 1.0907 | 1.0907 | H5 | 2.9316 | 1.0893 | 2.2306 | 2.2306 | | 1.7729 | 2.4776 | 3.0499 | 2.4776 | 3.0499 | H6 | 2.9337 | 1.0893 | 2.2307 | 2.2307 | 1.7729 | | 3.0492 | 2.4774 | 3.0492 | 2.4774 | H7 | 2.1373 | 2.2426 | 1.0907 | 2.8793 | 2.4776 | 3.0492 | | 1.7833 | 3.3635 | 3.8042 | H8 | 2.1373 | 2.2422 | 1.0907 | 2.8770 | 3.0499 | 2.4774 | 1.7833 | | 3.8042 | 3.3571 | H9 | 2.1373 | 2.2426 | 2.8793 | 1.0907 | 2.4776 | 3.0492 | 3.3635 | 3.8042 | | 1.7833 | H10 | 2.1373 | 2.2422 | 2.8770 | 1.0907 | 3.0499 | 2.4774 | 3.8042 | 3.3571 | 1.7833 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.334 |
|
O1 |
C3 |
H7 |
111.379 |
| O1 |
C3 |
H8 |
111.372 |
|
O1 |
C4 |
C2 |
91.334 |
| O1 |
C4 |
H9 |
111.379 |
|
O1 |
C4 |
H10 |
111.372 |
| C2 |
C3 |
H7 |
115.950 |
|
C2 |
C3 |
H8 |
115.914 |
| C2 |
C4 |
H9 |
115.950 |
|
C2 |
C4 |
H10 |
115.914 |
| C3 |
O1 |
C4 |
90.761 |
|
C3 |
C2 |
C4 |
86.572 |
| C3 |
C2 |
H5 |
115.021 |
|
C3 |
C2 |
H6 |
115.035 |
| C4 |
C2 |
H5 |
115.021 |
|
C4 |
C2 |
H6 |
115.035 |
| H5 |
C2 |
H6 |
108.933 |
|
H7 |
C3 |
H8 |
109.672 |
| H9 |
C4 |
H10 |
109.672 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.537 |
|
|
|
| 2 |
C |
-0.404 |
|
|
|
| 3 |
C |
-0.036 |
|
|
|
| 4 |
C |
-0.036 |
|
|
|
| 5 |
H |
0.176 |
|
|
|
| 6 |
H |
0.175 |
|
|
|
| 7 |
H |
0.165 |
|
|
|
| 8 |
H |
0.165 |
|
|
|
| 9 |
H |
0.165 |
|
|
|
| 10 |
H |
0.165 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.006 |
2.541 |
0.000 |
2.541 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.012 |
0.010 |
0.000 |
| y |
0.010 |
-28.339 |
0.000 |
| z |
0.000 |
0.000 |
-22.152 |
|
| Traceless |
| | x | y | z |
| x |
1.233 |
0.010 |
0.000 |
| y |
0.010 |
-5.257 |
0.000 |
| z |
0.000 |
0.000 |
4.024 |
|
| Polar |
| 3z2-r2 | 8.048 |
| x2-y2 | 4.327 |
| xy | 0.010 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.447 |
-0.000 |
0.000 |
| y |
-0.000 |
4.351 |
0.000 |
| z |
0.000 |
0.000 |
5.550 |
<r2> (average value of r
2) Å
2
| <r2> |
67.228 |
| (<r2>)1/2 |
8.199 |