Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-31G
| | hartrees |
| Energy at 0K | -192.759853 |
| Energy at 298.15K | -192.767021 |
| HF Energy | -192.625314 |
| Nuclear repulsion energy | 125.703307 |
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
| 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 |
3117 |
3117 |
18.20 |
|
|
|
| 2 |
A1 |
3100 |
3100 |
10.44 |
|
|
|
| 3 |
A1 |
1595 |
1595 |
0.10 |
|
|
|
| 4 |
A1 |
1554 |
1554 |
2.74 |
|
|
|
| 5 |
A1 |
1380 |
1380 |
0.18 |
|
|
|
| 6 |
A1 |
1023 |
1023 |
0.00 |
|
|
|
| 7 |
A1 |
853 |
853 |
12.71 |
|
|
|
| 8 |
A1 |
790 |
790 |
10.41 |
|
|
|
| 9 |
A2 |
3153 |
3153 |
0.00 |
|
|
|
| 10 |
A2 |
1274 |
1274 |
0.00 |
|
|
|
| 11 |
A2 |
1135 |
1135 |
0.00 |
|
|
|
| 12 |
A2 |
881 |
881 |
0.00 |
|
|
|
| 13 |
B1 |
3180 |
3180 |
75.07 |
|
|
|
| 14 |
B1 |
3148 |
3148 |
31.20 |
|
|
|
| 15 |
B1 |
1229 |
1229 |
2.24 |
|
|
|
| 16 |
B1 |
1120 |
1120 |
0.65 |
|
|
|
| 17 |
B1 |
797 |
797 |
0.73 |
|
|
|
| 18 |
B1 |
50 |
50 |
5.23 |
|
|
|
| 19 |
B2 |
3093 |
3093 |
110.11 |
|
|
|
| 20 |
B2 |
1572 |
1572 |
0.95 |
|
|
|
| 21 |
B2 |
1329 |
1329 |
13.43 |
|
|
|
| 22 |
B2 |
1310 |
1310 |
0.85 |
|
|
|
| 23 |
B2 |
981 |
981 |
12.61 |
|
|
|
| 24 |
B2 |
919 |
919 |
57.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19290.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19290.9 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
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.107 |
| C2 |
0.000 |
0.000 |
-1.077 |
| C3 |
0.000 |
1.069 |
0.047 |
| C4 |
0.000 |
-1.069 |
0.047 |
| H5 |
0.888 |
0.000 |
-1.711 |
| H6 |
-0.888 |
0.000 |
-1.711 |
| H7 |
0.894 |
1.692 |
0.115 |
| H8 |
-0.894 |
1.692 |
0.115 |
| H9 |
-0.894 |
-1.692 |
0.115 |
| H10 |
0.894 |
-1.692 |
0.115 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1841 | 1.5058 | 1.5058 | 2.9555 | 2.9555 | 2.1559 | 2.1559 | 2.1559 | 2.1559 |
C2 | 2.1841 | | 1.5507 | 1.5507 | 1.0918 | 1.0918 | 2.2548 | 2.2548 | 2.2548 | 2.2548 | C3 | 1.5058 | 1.5507 | | 2.1379 | 2.2412 | 2.2412 | 1.0923 | 1.0923 | 2.9032 | 2.9032 | C4 | 1.5058 | 1.5507 | 2.1379 | | 2.2412 | 2.2412 | 2.9032 | 2.9032 | 1.0923 | 1.0923 | H5 | 2.9555 | 1.0918 | 2.2412 | 2.2412 | | 1.7767 | 2.4901 | 3.0624 | 3.0624 | 2.4901 | H6 | 2.9555 | 1.0918 | 2.2412 | 2.2412 | 1.7767 | | 3.0624 | 2.4901 | 2.4901 | 3.0624 | H7 | 2.1559 | 2.2548 | 1.0923 | 2.9032 | 2.4901 | 3.0624 | | 1.7887 | 3.8281 | 3.3845 | H8 | 2.1559 | 2.2548 | 1.0923 | 2.9032 | 3.0624 | 2.4901 | 1.7887 | | 3.3845 | 3.8281 | H9 | 2.1559 | 2.2548 | 2.9032 | 1.0923 | 3.0624 | 2.4901 | 3.8281 | 3.3845 | | 1.7887 | H10 | 2.1559 | 2.2548 | 2.9032 | 1.0923 | 2.4901 | 3.0624 | 3.3845 | 3.8281 | 1.7887 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.201 |
|
O1 |
C3 |
H7 |
111.158 |
| O1 |
C3 |
H8 |
111.158 |
|
O1 |
C4 |
C2 |
91.201 |
| O1 |
C4 |
H9 |
111.158 |
|
O1 |
C4 |
H10 |
111.158 |
| C2 |
C3 |
H7 |
116.025 |
|
C2 |
C3 |
H8 |
116.025 |
| C2 |
C4 |
H9 |
116.025 |
|
C2 |
C4 |
H10 |
116.025 |
| C3 |
O1 |
C4 |
90.449 |
|
C3 |
C2 |
C4 |
87.150 |
| C3 |
C2 |
H5 |
114.909 |
|
C3 |
C2 |
H6 |
114.909 |
| C4 |
C2 |
H5 |
114.909 |
|
C4 |
C2 |
H6 |
114.909 |
| H5 |
C2 |
H6 |
108.908 |
|
H7 |
C3 |
H8 |
109.928 |
| H9 |
C4 |
H10 |
109.928 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-31G
| | hartrees |
| Energy at 0K | -192.759853 |
| Energy at 298.15K | -192.767023 |
| HF Energy | -192.625306 |
| Nuclear repulsion energy | 125.700851 |
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
| 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' |
3179 |
3179 |
75.85 |
|
|
|
| 2 |
A' |
3147 |
3147 |
30.40 |
|
|
|
| 3 |
A' |
3117 |
3117 |
18.02 |
|
|
|
| 4 |
A' |
3100 |
3100 |
10.66 |
|
|
|
| 5 |
A' |
1595 |
1595 |
0.10 |
|
|
|
| 6 |
A' |
1554 |
1554 |
2.73 |
|
|
|
| 7 |
A' |
1381 |
1381 |
0.18 |
|
|
|
| 8 |
A' |
1229 |
1229 |
2.24 |
|
|
|
| 9 |
A' |
1120 |
1120 |
0.65 |
|
|
|
| 10 |
A' |
1023 |
1023 |
0.00 |
|
|
|
| 11 |
A' |
853 |
853 |
12.66 |
|
|
|
| 12 |
A' |
797 |
797 |
0.86 |
|
|
|
| 13 |
A' |
790 |
790 |
10.32 |
|
|
|
| 14 |
A' |
51 |
51 |
5.23 |
|
|
|
| 15 |
A" |
3153 |
3153 |
0.00 |
|
|
|
| 16 |
A" |
3093 |
3093 |
110.07 |
|
|
|
| 17 |
A" |
1572 |
1572 |
0.94 |
|
|
|
| 18 |
A" |
1329 |
1329 |
13.48 |
|
|
|
| 19 |
A" |
1310 |
1310 |
0.79 |
|
|
|
| 20 |
A" |
1275 |
1275 |
0.00 |
|
|
|
| 21 |
A" |
1135 |
1135 |
0.00 |
|
|
|
| 22 |
A" |
981 |
981 |
12.30 |
|
|
|
| 23 |
A" |
918 |
918 |
57.40 |
|
|
|
| 24 |
A" |
881 |
881 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19290.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19290.9 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
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.003 |
-1.108 |
0.000 |
| C2 |
-0.001 |
1.077 |
0.000 |
| C3 |
-0.001 |
-0.047 |
1.069 |
| C4 |
-0.001 |
-0.047 |
-1.069 |
| H5 |
0.888 |
1.711 |
0.000 |
| H6 |
-0.889 |
1.712 |
0.000 |
| H7 |
0.892 |
-0.114 |
1.694 |
| H8 |
-0.896 |
-0.117 |
1.690 |
| H9 |
0.892 |
-0.114 |
-1.694 |
| H10 |
-0.896 |
-0.117 |
-1.690 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1842 | 1.5060 | 1.5060 | 2.9543 | 2.9572 | 2.1560 | 2.1560 | 2.1560 | 2.1560 |
C2 | 2.1842 | | 1.5506 | 1.5506 | 1.0919 | 1.0919 | 2.2550 | 2.2545 | 2.2550 | 2.2545 | C3 | 1.5060 | 1.5506 | | 2.1378 | 2.2410 | 2.2414 | 1.0923 | 1.0923 | 2.9047 | 2.9017 | C4 | 1.5060 | 1.5506 | 2.1378 | | 2.2410 | 2.2414 | 2.9047 | 2.9017 | 1.0923 | 1.0923 | H5 | 2.9543 | 1.0919 | 2.2410 | 2.2410 | | 1.7765 | 2.4903 | 3.0628 | 2.4903 | 3.0628 | H6 | 2.9572 | 1.0919 | 2.2414 | 2.2414 | 1.7765 | | 3.0620 | 2.4901 | 3.0620 | 2.4901 | H7 | 2.1560 | 2.2550 | 1.0923 | 2.9047 | 2.4903 | 3.0620 | | 1.7886 | 3.3885 | 3.8281 | H8 | 2.1560 | 2.2545 | 1.0923 | 2.9017 | 3.0628 | 2.4901 | 1.7886 | | 3.8281 | 3.3805 | H9 | 2.1560 | 2.2550 | 2.9047 | 1.0923 | 2.4903 | 3.0620 | 3.3885 | 3.8281 | | 1.7886 | H10 | 2.1560 | 2.2545 | 2.9017 | 1.0923 | 3.0628 | 2.4901 | 3.8281 | 3.3805 | 1.7886 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.205 |
|
O1 |
C3 |
H7 |
111.155 |
| O1 |
C3 |
H8 |
111.149 |
|
O1 |
C4 |
C2 |
91.205 |
| O1 |
C4 |
H9 |
111.155 |
|
O1 |
C4 |
H10 |
111.149 |
| C2 |
C3 |
H7 |
116.057 |
|
C2 |
C3 |
H8 |
116.009 |
| C2 |
C4 |
H9 |
116.057 |
|
C2 |
C4 |
H10 |
116.009 |
| C3 |
O1 |
C4 |
90.431 |
|
C3 |
C2 |
C4 |
87.159 |
| C3 |
C2 |
H5 |
114.904 |
|
C3 |
C2 |
H6 |
114.930 |
| C4 |
C2 |
H5 |
114.904 |
|
C4 |
C2 |
H6 |
114.930 |
| H5 |
C2 |
H6 |
108.877 |
|
H7 |
C3 |
H8 |
109.922 |
| H9 |
C4 |
H10 |
109.922 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability