Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -192.935263 |
| Energy at 298.15K | |
| HF Energy | -192.723456 |
| Nuclear repulsion energy | 127.478998 |
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-pVDZ
| 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 |
3108 |
2991 |
27.86 |
|
|
|
| 2 |
A1 |
3061 |
2946 |
0.24 |
|
|
|
| 3 |
A1 |
1538 |
1480 |
0.00 |
|
|
|
| 4 |
A1 |
1490 |
1434 |
3.33 |
|
|
|
| 5 |
A1 |
1361 |
1309 |
1.32 |
|
|
|
| 6 |
A1 |
1045 |
1006 |
3.98 |
|
|
|
| 7 |
A1 |
918 |
883 |
34.12 |
|
|
|
| 8 |
A1 |
808 |
777 |
6.65 |
|
|
|
| 9 |
A2 |
3109 |
2992 |
0.00 |
|
|
|
| 10 |
A2 |
1233 |
1186 |
0.00 |
|
|
|
| 11 |
A2 |
1153 |
1109 |
0.00 |
|
|
|
| 12 |
A2 |
834 |
803 |
0.00 |
|
|
|
| 13 |
B1 |
3170 |
3050 |
34.70 |
|
|
|
| 14 |
B1 |
3107 |
2990 |
60.76 |
|
|
|
| 15 |
B1 |
1193 |
1148 |
0.23 |
|
|
|
| 16 |
B1 |
1138 |
1096 |
1.81 |
|
|
|
| 17 |
B1 |
765 |
736 |
0.14 |
|
|
|
| 18 |
B1 |
38i |
37i |
4.09 |
|
|
|
| 19 |
B2 |
3054 |
2939 |
151.11 |
|
|
|
| 20 |
B2 |
1511 |
1454 |
0.83 |
|
|
|
| 21 |
B2 |
1299 |
1250 |
0.58 |
|
|
|
| 22 |
B2 |
1250 |
1203 |
6.14 |
|
|
|
| 23 |
B2 |
1020 |
982 |
88.17 |
|
|
|
| 24 |
B2 |
951 |
915 |
11.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19038.3 cm
-1
Scaled (by 0.9623) Zero Point Vibrational Energy (zpe) 18320.5 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-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.077 |
| C2 |
0.000 |
0.000 |
-1.077 |
| C3 |
0.000 |
1.043 |
0.060 |
| C4 |
0.000 |
-1.043 |
0.060 |
| H5 |
0.895 |
0.000 |
-1.708 |
| H6 |
-0.895 |
0.000 |
-1.708 |
| H7 |
0.898 |
1.673 |
0.135 |
| H8 |
-0.898 |
1.673 |
0.135 |
| H9 |
-0.898 |
-1.673 |
0.135 |
| H10 |
0.898 |
-1.673 |
0.135 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1541 | 1.4571 | 1.4571 | 2.9253 | 2.9253 | 2.1195 | 2.1195 | 2.1195 | 2.1195 |
C2 | 2.1541 | | 1.5434 | 1.5434 | 1.0948 | 1.0948 | 2.2526 | 2.2526 | 2.2526 | 2.2526 | C3 | 1.4571 | 1.5434 | | 2.0869 | 2.2396 | 2.2396 | 1.0991 | 1.0991 | 2.8620 | 2.8620 | C4 | 1.4571 | 1.5434 | 2.0869 | | 2.2396 | 2.2396 | 2.8620 | 2.8620 | 1.0991 | 1.0991 | H5 | 2.9253 | 1.0948 | 2.2396 | 2.2396 | | 1.7891 | 2.4893 | 3.0674 | 3.0674 | 2.4893 | H6 | 2.9253 | 1.0948 | 2.2396 | 2.2396 | 1.7891 | | 3.0674 | 2.4893 | 2.4893 | 3.0674 | H7 | 2.1195 | 2.2526 | 1.0991 | 2.8620 | 2.4893 | 3.0674 | | 1.7956 | 3.7974 | 3.3460 | H8 | 2.1195 | 2.2526 | 1.0991 | 2.8620 | 3.0674 | 2.4893 | 1.7956 | | 3.3460 | 3.7974 | H9 | 2.1195 | 2.2526 | 2.8620 | 1.0991 | 3.0674 | 2.4893 | 3.7974 | 3.3460 | | 1.7956 | H10 | 2.1195 | 2.2526 | 2.8620 | 1.0991 | 2.4893 | 3.0674 | 3.3460 | 3.7974 | 1.7956 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.723 |
|
O1 |
C3 |
H7 |
111.257 |
| O1 |
C3 |
H8 |
111.257 |
|
O1 |
C4 |
C2 |
91.723 |
| O1 |
C4 |
H9 |
111.257 |
|
O1 |
C4 |
H10 |
111.257 |
| C2 |
C3 |
H7 |
115.948 |
|
C2 |
C3 |
H8 |
115.948 |
| C2 |
C4 |
H9 |
115.948 |
|
C2 |
C4 |
H10 |
115.948 |
| C3 |
O1 |
C4 |
91.474 |
|
C3 |
C2 |
C4 |
85.080 |
| C3 |
C2 |
H5 |
115.134 |
|
C3 |
C2 |
H6 |
115.134 |
| C4 |
C2 |
H5 |
115.134 |
|
C4 |
C2 |
H6 |
115.134 |
| H5 |
C2 |
H6 |
109.596 |
|
H7 |
C3 |
H8 |
109.544 |
| H9 |
C4 |
H10 |
109.544 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -192.935270 |
| Energy at 298.15K | |
| HF Energy | -192.723410 |
| Nuclear repulsion energy | 127.529361 |
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-pVDZ
| 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' |
3169 |
3050 |
35.28 |
|
|
|
| 2 |
A' |
3110 |
2993 |
46.44 |
|
|
|
| 3 |
A' |
3105 |
2988 |
35.44 |
|
|
|
| 4 |
A' |
3059 |
2944 |
8.62 |
|
|
|
| 5 |
A' |
1538 |
1480 |
0.02 |
|
|
|
| 6 |
A' |
1490 |
1434 |
3.31 |
|
|
|
| 7 |
A' |
1360 |
1309 |
1.30 |
|
|
|
| 8 |
A' |
1194 |
1149 |
0.20 |
|
|
|
| 9 |
A' |
1141 |
1098 |
2.05 |
|
|
|
| 10 |
A' |
1046 |
1007 |
4.32 |
|
|
|
| 11 |
A' |
917 |
883 |
32.95 |
|
|
|
| 12 |
A' |
823 |
792 |
7.57 |
|
|
|
| 13 |
A' |
749 |
721 |
0.67 |
|
|
|
| 14 |
A' |
55 |
53 |
4.16 |
|
|
|
| 15 |
A" |
3111 |
2994 |
6.42 |
|
|
|
| 16 |
A" |
3052 |
2937 |
142.67 |
|
|
|
| 17 |
A" |
1510 |
1453 |
0.81 |
|
|
|
| 18 |
A" |
1299 |
1251 |
0.61 |
|
|
|
| 19 |
A" |
1253 |
1206 |
4.90 |
|
|
|
| 20 |
A" |
1229 |
1182 |
1.39 |
|
|
|
| 21 |
A" |
1151 |
1108 |
0.13 |
|
|
|
| 22 |
A" |
1018 |
979 |
87.35 |
|
|
|
| 23 |
A" |
951 |
915 |
9.89 |
|
|
|
| 24 |
A" |
833 |
802 |
0.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19081.8 cm
-1
Scaled (by 0.9623) Zero Point Vibrational Energy (zpe) 18362.4 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/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.104 |
-1.072 |
0.000 |
| C2 |
-0.028 |
1.076 |
0.000 |
| C3 |
-0.028 |
-0.062 |
1.042 |
| C4 |
-0.028 |
-0.062 |
-1.042 |
| H5 |
0.881 |
1.686 |
0.000 |
| H6 |
-0.908 |
1.728 |
0.000 |
| H7 |
0.819 |
-0.093 |
1.740 |
| H8 |
-0.969 |
-0.187 |
1.598 |
| H9 |
0.819 |
-0.093 |
-1.740 |
| H10 |
-0.969 |
-0.187 |
-1.598 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1519 | 1.4570 | 1.4570 | 2.8646 | 2.9772 | 2.1203 | 2.1188 | 2.1203 | 2.1188 |
C2 | 2.1519 | | 1.5429 | 1.5429 | 1.0948 | 1.0949 | 2.2610 | 2.2438 | 2.2610 | 2.2438 | C3 | 1.4570 | 1.5429 | | 2.0838 | 2.2285 | 2.2502 | 1.0983 | 1.0999 | 2.9081 | 2.8056 | C4 | 1.4570 | 1.5429 | 2.0838 | | 2.2285 | 2.2502 | 2.9081 | 2.8056 | 1.0983 | 1.0999 | H5 | 2.8646 | 1.0948 | 2.2285 | 2.2285 | | 1.7897 | 2.4888 | 3.0796 | 2.4888 | 3.0796 | H6 | 2.9772 | 1.0949 | 2.2502 | 2.2502 | 1.7897 | | 3.0539 | 2.4952 | 3.0539 | 2.4952 | H7 | 2.1203 | 2.2610 | 1.0983 | 2.9081 | 2.4888 | 3.0539 | | 1.7960 | 3.4796 | 3.7880 | H8 | 2.1188 | 2.2438 | 1.0999 | 2.8056 | 3.0796 | 2.4952 | 1.7960 | | 3.7880 | 3.1968 | H9 | 2.1203 | 2.2610 | 2.9081 | 1.0983 | 2.4888 | 3.0539 | 3.4796 | 3.7880 | | 1.7960 | H10 | 2.1188 | 2.2438 | 2.8056 | 1.0999 | 3.0796 | 2.4952 | 3.7880 | 3.1968 | 1.7960 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.623 |
|
O1 |
C3 |
H7 |
111.375 |
| O1 |
C3 |
H8 |
111.153 |
|
O1 |
C4 |
C2 |
91.623 |
| O1 |
C4 |
H9 |
111.375 |
|
O1 |
C4 |
H10 |
111.153 |
| C2 |
C3 |
H7 |
116.745 |
|
C2 |
C3 |
H8 |
115.184 |
| C2 |
C4 |
H9 |
116.745 |
|
C2 |
C4 |
H10 |
115.184 |
| C3 |
O1 |
C4 |
91.300 |
|
C3 |
C2 |
C4 |
84.950 |
| C3 |
C2 |
H5 |
114.240 |
|
C3 |
C2 |
H6 |
116.055 |
| C4 |
C2 |
H5 |
114.240 |
|
C4 |
C2 |
H6 |
116.055 |
| H5 |
C2 |
H6 |
109.627 |
|
H7 |
C3 |
H8 |
109.573 |
| H9 |
C4 |
H10 |
109.573 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability