Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -192.952635 |
| Energy at 298.15K | -192.959812 |
| HF Energy | -192.716143 |
| Nuclear repulsion energy | 128.284126 |
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/6-31G(2df,p)
| 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 |
3122 |
3122 |
23.13 |
|
|
|
| 2 |
A1 |
3060 |
3060 |
1.31 |
|
|
|
| 3 |
A1 |
1565 |
1565 |
0.00 |
|
|
|
| 4 |
A1 |
1510 |
1510 |
1.66 |
|
|
|
| 5 |
A1 |
1396 |
1396 |
3.55 |
|
|
|
| 6 |
A1 |
1063 |
1063 |
5.20 |
|
|
|
| 7 |
A1 |
942 |
942 |
25.94 |
|
|
|
| 8 |
A1 |
821 |
821 |
4.52 |
|
|
|
| 9 |
A2 |
3100 |
3100 |
0.00 |
|
|
|
| 10 |
A2 |
1252 |
1252 |
0.00 |
|
|
|
| 11 |
A2 |
1179 |
1179 |
0.00 |
|
|
|
| 12 |
A2 |
843 |
843 |
0.00 |
|
|
|
| 13 |
B1 |
3181 |
3181 |
26.21 |
|
|
|
| 14 |
B1 |
3099 |
3099 |
74.97 |
|
|
|
| 15 |
B1 |
1210 |
1210 |
0.44 |
|
|
|
| 16 |
B1 |
1161 |
1161 |
2.20 |
|
|
|
| 17 |
B1 |
770 |
770 |
0.18 |
|
|
|
| 18 |
B1 |
30 |
30 |
2.81 |
|
|
|
| 19 |
B2 |
3051 |
3051 |
143.22 |
|
|
|
| 20 |
B2 |
1536 |
1536 |
3.78 |
|
|
|
| 21 |
B2 |
1326 |
1326 |
0.06 |
|
|
|
| 22 |
B2 |
1273 |
1273 |
5.49 |
|
|
|
| 23 |
B2 |
1054 |
1054 |
93.21 |
|
|
|
| 24 |
B2 |
960 |
960 |
6.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19251.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19251.6 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/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.069 |
| C2 |
0.000 |
0.000 |
-1.075 |
| C3 |
0.000 |
1.034 |
0.065 |
| C4 |
0.000 |
-1.034 |
0.065 |
| H5 |
0.888 |
0.000 |
-1.704 |
| H6 |
-0.888 |
0.000 |
-1.704 |
| H7 |
0.890 |
1.667 |
0.132 |
| H8 |
-0.890 |
1.667 |
0.132 |
| H9 |
-0.890 |
-1.667 |
0.132 |
| H10 |
0.890 |
-1.667 |
0.132 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1445 | 1.4417 | 1.4417 | 2.9120 | 2.9120 | 2.1089 | 2.1089 | 2.1089 | 2.1089 |
C2 | 2.1445 | | 1.5391 | 1.5391 | 1.0881 | 1.0881 | 2.2423 | 2.2423 | 2.2423 | 2.2423 | C3 | 1.4417 | 1.5391 | | 2.0682 | 2.2330 | 2.2330 | 1.0939 | 1.0939 | 2.8444 | 2.8444 | C4 | 1.4417 | 1.5391 | 2.0682 | | 2.2330 | 2.2330 | 2.8444 | 2.8444 | 1.0939 | 1.0939 | H5 | 2.9120 | 1.0881 | 2.2330 | 2.2330 | | 1.7759 | 2.4799 | 3.0514 | 3.0514 | 2.4799 | H6 | 2.9120 | 1.0881 | 2.2330 | 2.2330 | 1.7759 | | 3.0514 | 2.4799 | 2.4799 | 3.0514 | H7 | 2.1089 | 2.2423 | 1.0939 | 2.8444 | 2.4799 | 3.0514 | | 1.7799 | 3.7787 | 3.3333 | H8 | 2.1089 | 2.2423 | 1.0939 | 2.8444 | 3.0514 | 2.4799 | 1.7799 | | 3.3333 | 3.7787 | H9 | 2.1089 | 2.2423 | 2.8444 | 1.0939 | 3.0514 | 2.4799 | 3.7787 | 3.3333 | | 1.7799 | H10 | 2.1089 | 2.2423 | 2.8444 | 1.0939 | 2.4799 | 3.0514 | 3.3333 | 3.7787 | 1.7799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.956 |
|
O1 |
C3 |
H7 |
111.821 |
| O1 |
C3 |
H8 |
111.821 |
|
O1 |
C4 |
C2 |
91.956 |
| O1 |
C4 |
H9 |
111.821 |
|
O1 |
C4 |
H10 |
111.821 |
| C2 |
C3 |
H7 |
115.739 |
|
C2 |
C3 |
H8 |
115.739 |
| C2 |
C4 |
H9 |
115.739 |
|
C2 |
C4 |
H10 |
115.739 |
| C3 |
O1 |
C4 |
91.663 |
|
C3 |
C2 |
C4 |
84.426 |
| C3 |
C2 |
H5 |
115.343 |
|
C3 |
C2 |
H6 |
115.343 |
| C4 |
C2 |
H5 |
115.343 |
|
C4 |
C2 |
H6 |
115.343 |
| H5 |
C2 |
H6 |
109.391 |
|
H7 |
C3 |
H8 |
108.885 |
| H9 |
C4 |
H10 |
108.885 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -192.952635 |
| Energy at 298.15K | -192.959813 |
| HF Energy | -192.716143 |
| Nuclear repulsion energy | 128.285390 |
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/6-31G(2df,p)
| 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' |
3181 |
3181 |
26.28 |
|
|
|
| 2 |
A' |
3122 |
3122 |
23.15 |
|
|
|
| 3 |
A' |
3099 |
3099 |
74.92 |
|
|
|
| 4 |
A' |
3060 |
3060 |
1.31 |
|
|
|
| 5 |
A' |
1565 |
1565 |
0.00 |
|
|
|
| 6 |
A' |
1510 |
1510 |
1.66 |
|
|
|
| 7 |
A' |
1396 |
1396 |
3.55 |
|
|
|
| 8 |
A' |
1210 |
1210 |
0.44 |
|
|
|
| 9 |
A' |
1160 |
1160 |
2.20 |
|
|
|
| 10 |
A' |
1064 |
1064 |
5.20 |
|
|
|
| 11 |
A' |
942 |
942 |
25.94 |
|
|
|
| 12 |
A' |
821 |
821 |
4.51 |
|
|
|
| 13 |
A' |
770 |
770 |
0.18 |
|
|
|
| 14 |
A' |
30 |
30 |
2.81 |
|
|
|
| 15 |
A" |
3100 |
3100 |
0.00 |
|
|
|
| 16 |
A" |
3051 |
3051 |
143.22 |
|
|
|
| 17 |
A" |
1536 |
1536 |
3.78 |
|
|
|
| 18 |
A" |
1326 |
1326 |
0.06 |
|
|
|
| 19 |
A" |
1274 |
1274 |
5.48 |
|
|
|
| 20 |
A" |
1252 |
1252 |
0.00 |
|
|
|
| 21 |
A" |
1179 |
1179 |
0.00 |
|
|
|
| 22 |
A" |
1055 |
1055 |
93.21 |
|
|
|
| 23 |
A" |
960 |
960 |
6.36 |
|
|
|
| 24 |
A" |
843 |
843 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19251.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19251.8 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.000 |
-1.069 |
0.000 |
| C2 |
0.000 |
1.075 |
0.000 |
| C3 |
0.000 |
-0.065 |
1.034 |
| C4 |
0.000 |
-0.065 |
-1.034 |
| H5 |
0.888 |
1.704 |
0.000 |
| H6 |
-0.888 |
1.704 |
0.000 |
| H7 |
0.890 |
-0.132 |
1.666 |
| H8 |
-0.890 |
-0.132 |
1.667 |
| H9 |
0.890 |
-0.132 |
-1.666 |
| H10 |
-0.890 |
-0.132 |
-1.667 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1444 | 1.4417 | 1.4417 | 2.9123 | 2.9117 | 2.1090 | 2.1090 | 2.1090 | 2.1090 |
C2 | 2.1444 | | 1.5391 | 1.5391 | 1.0881 | 1.0881 | 2.2422 | 2.2423 | 2.2422 | 2.2423 | C3 | 1.4417 | 1.5391 | | 2.0683 | 2.2332 | 2.2330 | 1.0939 | 1.0939 | 2.8443 | 2.8447 | C4 | 1.4417 | 1.5391 | 2.0683 | | 2.2332 | 2.2330 | 2.8443 | 2.8447 | 1.0939 | 1.0939 | H5 | 2.9123 | 1.0881 | 2.2332 | 2.2332 | | 1.7757 | 2.4800 | 3.0513 | 2.4800 | 3.0513 | H6 | 2.9117 | 1.0881 | 2.2330 | 2.2330 | 1.7757 | | 3.0514 | 2.4799 | 3.0514 | 2.4799 | H7 | 2.1090 | 2.2422 | 1.0939 | 2.8443 | 2.4800 | 3.0514 | | 1.7799 | 3.3328 | 3.7788 | H8 | 2.1090 | 2.2423 | 1.0939 | 2.8447 | 3.0513 | 2.4799 | 1.7799 | | 3.7788 | 3.3340 | H9 | 2.1090 | 2.2422 | 2.8443 | 1.0939 | 2.4800 | 3.0514 | 3.3328 | 3.7788 | | 1.7799 | H10 | 2.1090 | 2.2423 | 2.8447 | 1.0939 | 3.0513 | 2.4799 | 3.7788 | 3.3340 | 1.7799 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.951 |
|
O1 |
C3 |
H7 |
111.826 |
| O1 |
C3 |
H8 |
111.825 |
|
O1 |
C4 |
C2 |
91.951 |
| O1 |
C4 |
H9 |
111.826 |
|
O1 |
C4 |
H10 |
111.825 |
| C2 |
C3 |
H7 |
115.732 |
|
C2 |
C3 |
H8 |
115.742 |
| C2 |
C4 |
H9 |
115.732 |
|
C2 |
C4 |
H10 |
115.742 |
| C3 |
O1 |
C4 |
91.668 |
|
C3 |
C2 |
C4 |
84.431 |
| C3 |
C2 |
H5 |
115.355 |
|
C3 |
C2 |
H6 |
115.342 |
| C4 |
C2 |
H5 |
115.355 |
|
C4 |
C2 |
H6 |
115.342 |
| H5 |
C2 |
H6 |
109.371 |
|
H7 |
C3 |
H8 |
108.885 |
| H9 |
C4 |
H10 |
108.885 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability