Jump to
S1C2
Energy calculated at B2PLYP=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -192.908807 |
| Energy at 298.15K | -192.915983 |
| HF Energy | -192.708089 |
| Nuclear repulsion energy | 127.825300 |
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=FULL/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 |
3107 |
2978 |
25.68 |
|
|
|
| 2 |
A1 |
3049 |
2923 |
2.70 |
|
|
|
| 3 |
A1 |
1539 |
1475 |
0.01 |
|
|
|
| 4 |
A1 |
1480 |
1418 |
2.54 |
|
|
|
| 5 |
A1 |
1383 |
1326 |
4.65 |
|
|
|
| 6 |
A1 |
1061 |
1017 |
5.99 |
|
|
|
| 7 |
A1 |
939 |
900 |
28.06 |
|
|
|
| 8 |
A1 |
824 |
790 |
4.37 |
|
|
|
| 9 |
A2 |
3091 |
2963 |
0.00 |
|
|
|
| 10 |
A2 |
1235 |
1183 |
0.00 |
|
|
|
| 11 |
A2 |
1164 |
1116 |
0.00 |
|
|
|
| 12 |
A2 |
840 |
805 |
0.00 |
|
|
|
| 13 |
B1 |
3169 |
3037 |
32.23 |
|
|
|
| 14 |
B1 |
3090 |
2961 |
90.27 |
|
|
|
| 15 |
B1 |
1193 |
1144 |
0.62 |
|
|
|
| 16 |
B1 |
1146 |
1098 |
2.30 |
|
|
|
| 17 |
B1 |
764 |
733 |
0.24 |
|
|
|
| 18 |
B1 |
33 |
31 |
2.27 |
|
|
|
| 19 |
B2 |
3039 |
2913 |
159.93 |
|
|
|
| 20 |
B2 |
1508 |
1445 |
3.86 |
|
|
|
| 21 |
B2 |
1310 |
1256 |
0.07 |
|
|
|
| 22 |
B2 |
1265 |
1213 |
4.70 |
|
|
|
| 23 |
B2 |
1052 |
1008 |
97.24 |
|
|
|
| 24 |
B2 |
959 |
919 |
7.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19118.8 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 18325.4 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=FULL/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.072 |
| C2 |
0.000 |
0.000 |
-1.076 |
| C3 |
0.000 |
1.037 |
0.065 |
| C4 |
0.000 |
-1.037 |
0.065 |
| H5 |
0.895 |
0.000 |
-1.711 |
| H6 |
-0.895 |
0.000 |
-1.711 |
| H7 |
0.897 |
1.676 |
0.131 |
| H8 |
-0.897 |
1.676 |
0.131 |
| H9 |
-0.897 |
-1.676 |
0.131 |
| H10 |
0.897 |
-1.676 |
0.131 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1480 | 1.4453 | 1.4453 | 2.9232 | 2.9232 | 2.1206 | 2.1206 | 2.1206 | 2.1206 |
C2 | 2.1480 | | 1.5416 | 1.5416 | 1.0976 | 1.0976 | 2.2515 | 2.2515 | 2.2515 | 2.2515 | C3 | 1.4453 | 1.5416 | | 2.0734 | 2.2426 | 2.2426 | 1.1032 | 1.1032 | 2.8575 | 2.8575 | C4 | 1.4453 | 1.5416 | 2.0734 | | 2.2426 | 2.2426 | 2.8575 | 2.8575 | 1.1032 | 1.1032 | H5 | 2.9232 | 1.0976 | 2.2426 | 2.2426 | | 1.7909 | 2.4900 | 3.0680 | 3.0680 | 2.4900 | H6 | 2.9232 | 1.0976 | 2.2426 | 2.2426 | 1.7909 | | 3.0680 | 2.4900 | 2.4900 | 3.0680 | H7 | 2.1206 | 2.2515 | 1.1032 | 2.8575 | 2.4900 | 3.0680 | | 1.7938 | 3.8010 | 3.3512 | H8 | 2.1206 | 2.2515 | 1.1032 | 2.8575 | 3.0680 | 2.4900 | 1.7938 | | 3.3512 | 3.8010 | H9 | 2.1206 | 2.2515 | 2.8575 | 1.1032 | 3.0680 | 2.4900 | 3.8010 | 3.3512 | | 1.7938 | H10 | 2.1206 | 2.2515 | 2.8575 | 1.1032 | 2.4900 | 3.0680 | 3.3512 | 3.8010 | 1.7938 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.910 |
|
O1 |
C3 |
H7 |
111.932 |
| O1 |
C3 |
H8 |
111.932 |
|
O1 |
C4 |
C2 |
91.910 |
| O1 |
C4 |
H9 |
111.932 |
|
O1 |
C4 |
H10 |
111.932 |
| C2 |
C3 |
H7 |
115.719 |
|
C2 |
C3 |
H8 |
115.719 |
| C2 |
C4 |
H9 |
115.719 |
|
C2 |
C4 |
H10 |
115.719 |
| C3 |
O1 |
C4 |
91.659 |
|
C3 |
C2 |
C4 |
84.521 |
| C3 |
C2 |
H5 |
115.338 |
|
C3 |
C2 |
H6 |
115.338 |
| C4 |
C2 |
H5 |
115.338 |
|
C4 |
C2 |
H6 |
115.338 |
| H5 |
C2 |
H6 |
109.345 |
|
H7 |
C3 |
H8 |
108.784 |
| H9 |
C4 |
H10 |
108.784 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -192.908807 |
| Energy at 298.15K | -192.915983 |
| HF Energy | -192.708089 |
| Nuclear repulsion energy | 127.824925 |
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=FULL/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 |
3037 |
32.32 |
|
|
|
| 2 |
A' |
3107 |
2978 |
25.70 |
|
|
|
| 3 |
A' |
3090 |
2961 |
90.17 |
|
|
|
| 4 |
A' |
3049 |
2923 |
2.71 |
|
|
|
| 5 |
A' |
1539 |
1475 |
0.01 |
|
|
|
| 6 |
A' |
1480 |
1418 |
2.54 |
|
|
|
| 7 |
A' |
1383 |
1326 |
4.65 |
|
|
|
| 8 |
A' |
1193 |
1143 |
0.62 |
|
|
|
| 9 |
A' |
1146 |
1098 |
2.30 |
|
|
|
| 10 |
A' |
1061 |
1017 |
5.98 |
|
|
|
| 11 |
A' |
939 |
900 |
28.07 |
|
|
|
| 12 |
A' |
824 |
790 |
4.37 |
|
|
|
| 13 |
A' |
764 |
733 |
0.24 |
|
|
|
| 14 |
A' |
33 |
32 |
2.27 |
|
|
|
| 15 |
A" |
3091 |
2963 |
0.00 |
|
|
|
| 16 |
A" |
3039 |
2913 |
159.90 |
|
|
|
| 17 |
A" |
1508 |
1445 |
3.86 |
|
|
|
| 18 |
A" |
1310 |
1255 |
0.07 |
|
|
|
| 19 |
A" |
1265 |
1213 |
4.69 |
|
|
|
| 20 |
A" |
1235 |
1183 |
0.00 |
|
|
|
| 21 |
A" |
1164 |
1116 |
0.00 |
|
|
|
| 22 |
A" |
1052 |
1008 |
97.24 |
|
|
|
| 23 |
A" |
959 |
919 |
7.51 |
|
|
|
| 24 |
A" |
840 |
805 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19118.9 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 18325.5 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=FULL/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.001 |
-1.072 |
0.000 |
| C2 |
-0.000 |
1.076 |
0.000 |
| C3 |
-0.000 |
-0.065 |
1.037 |
| C4 |
-0.000 |
-0.065 |
-1.037 |
| H5 |
0.895 |
1.711 |
0.000 |
| H6 |
-0.895 |
1.711 |
0.000 |
| H7 |
0.896 |
-0.131 |
1.676 |
| H8 |
-0.897 |
-0.131 |
1.675 |
| H9 |
0.896 |
-0.131 |
-1.676 |
| H10 |
-0.897 |
-0.131 |
-1.675 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1479 | 1.4453 | 1.4453 | 2.9229 | 2.9236 | 2.1207 | 2.1207 | 2.1207 | 2.1207 |
C2 | 2.1479 | | 1.5416 | 1.5416 | 1.0976 | 1.0976 | 2.2515 | 2.2514 | 2.2515 | 2.2514 | C3 | 1.4453 | 1.5416 | | 2.0734 | 2.2426 | 2.2427 | 1.1032 | 1.1032 | 2.8579 | 2.8572 | C4 | 1.4453 | 1.5416 | 2.0734 | | 2.2426 | 2.2427 | 2.8579 | 2.8572 | 1.1032 | 1.1032 | H5 | 2.9229 | 1.0976 | 2.2426 | 2.2426 | | 1.7908 | 2.4900 | 3.0681 | 2.4900 | 3.0681 | H6 | 2.9236 | 1.0976 | 2.2427 | 2.2427 | 1.7908 | | 3.0679 | 2.4900 | 3.0679 | 2.4900 | H7 | 2.1207 | 2.2515 | 1.1032 | 2.8579 | 2.4900 | 3.0679 | | 1.7938 | 3.3521 | 3.8011 | H8 | 2.1207 | 2.2514 | 1.1032 | 2.8572 | 3.0681 | 2.4900 | 1.7938 | | 3.8011 | 3.3503 | H9 | 2.1207 | 2.2515 | 2.8579 | 1.1032 | 2.4900 | 3.0679 | 3.3521 | 3.8011 | | 1.7938 | H10 | 2.1207 | 2.2514 | 2.8572 | 1.1032 | 3.0681 | 2.4900 | 3.8011 | 3.3503 | 1.7938 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.907 |
|
O1 |
C3 |
H7 |
111.937 |
| O1 |
C3 |
H8 |
111.934 |
|
O1 |
C4 |
C2 |
91.907 |
| O1 |
C4 |
H9 |
111.937 |
|
O1 |
C4 |
H10 |
111.934 |
| C2 |
C3 |
H7 |
115.719 |
|
C2 |
C3 |
H8 |
115.711 |
| C2 |
C4 |
H9 |
115.719 |
|
C2 |
C4 |
H10 |
115.711 |
| C3 |
O1 |
C4 |
91.662 |
|
C3 |
C2 |
C4 |
84.523 |
| C3 |
C2 |
H5 |
115.339 |
|
C3 |
C2 |
H6 |
115.347 |
| C4 |
C2 |
H5 |
115.339 |
|
C4 |
C2 |
H6 |
115.347 |
| H5 |
C2 |
H6 |
109.328 |
|
H7 |
C3 |
H8 |
108.787 |
| H9 |
C4 |
H10 |
108.787 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability